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YUN, GUNSU (윤건수)

Div. of Advanced Nuclear Engineering(첨단원자력공학부)

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DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||DENSITY:4||FUSION PLASMAS:4||DIAGNOSTICS:3||TOKAMAK:3||TRANSPORT:3||TURBULENCE:3||REFLECTOMETRY:3||Plasma diagnostics  interferometry, spectroscopy and imaging:3||PLASMAS:3||MAGNETIC RECONNECTION:2||FLUCTUATION MEASUREMENTS:2||DIIID:2||ASDEX UPGRADE:2||Shear flow:2||CONFINEMENT:2||Plasma diagnostics:2||electron cyclotron emission:2||Nuclear instruments and methods for hot plasma diagnostics:2||Magnetoplasma:2||ANTENNAARRAYS:2||SAWTOOTH OSCILLATION:2||TEMPERATUREFLUCTUATIONS:2||MILLIMETERWAVE:2||TOROIDALMOMENTUM DISSIPATION:2||ECE:2||ECEI:1||MICROWAVE IMAGING REFLECTOMETRY:1||ELECTRONCYCLOTRON EMISSION:1||INJECTION:1||Edge localized modes:1||FLOWS:1||LARGE HELICAL DEVICE:1||Global modeling:1||ELM PRECURSORS:1||ELMs:1||DOPPLER REFLECTOMETRY:1||HMODE:1||FREQUENCY CONTROL:1||plasma temperature:1||DISRUPTIONS:1||Complex GinzburgLandau equation:1||Dynamical features:1||Quasisteady state:1||Imaging systems:1||Reflectometers:1||TOKAMAK PLASMAS:1||FACILITY ATF TORSATRON:1||Linearly polarized:1||Instantaneous power densities:1||Plasma disruption:1||synthetic diagnostics:1||Radiation calculations:1||ROTATION:1||plasma confinement:1||DIIID TOKAMAK:1||Microwave diagnostics:1||reflectometry:1||INSTABILITIES:1||MITIGATION:1||Plasma stability:1||Korea superconducting tokamak advanced researches:1||Particle beam injection:1||Neutral beam injection:1||PROJECT:1||ENERGY CONFINEMENT:1||DENSITYFLUCTUATIONS:1||Ionization of gases:1||Delay dependent:1||Argon:1||Resonators:1||Microwave pulse:1||Wave plasma interactions:1||Displacement direction:1||Magnetic perturbation:1||Sawtooth crashes:1||Millimeterwave radiometry:1||ENERGY:1||millimeterwave imaging:1||IONIZEDGAS:1||SPECTROSCOPY:1||MODE POWER THRESHOLD:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||Timevarying plasma:1||ABSORPTION:1||MAGNETIC SHEAR:1||CHAPTER 1:1||ITER:1||IMPROVED CONFINEMENT:1||SYSTEM:1||Filamentary structures:1||Hightemperature plasmas:1||Dominant mode:1||Gyroscale:1||WAVES:1||PLASMA MICROINSTABILITIES:1||Time delay:1||Collisional plasmas:1||Density of electrons:1||Source of electrons:1||Sawtooth periods:1||EDGE LOCALIZED MODES:1||spatial resolution:1||NSTX:1||RECONNECTION:1||Nonlinear stabilities:1||Linear growth rate:1||Plasma simulation:1||PERTURBATIONS:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||Plasma Physics:1||Impedance mismatch:1||Magnetohydrodynamics:1||Spatial orientations:1||PENETRATION:1||BOUT plus:1||KSTAR:1||PEDESTAL:1||ECE imaging system:1||refraction effect:1||pressure effect:1||TOKAMAKS:1||DISCHARGES:1||plasma transport processes:1||PLASMACONFINEMENT:1||REGIME:1||ALFVEN EIGENMODE:1||MICROTURBULENCE:1||electron confinement, energetic electron, microplasma, microwave discharge, pulse discharge:1||Tokamak devices:1||ELMS:1||FLUID KINETIC DESCRIPTION:1||Collision dynamics:1||Microwave resonators:1||Strong correlation:1||TEMPERATURE:1||REVERSED SHEAR PLASMAS:1||RADIAL ELECTRICFIELD:1||PARAMETERS:1||HEATED DIVERTOR DISCHARGES:1||TCV:1||TOROIDAL PLASMAS:1||Density fluctuation:1||Gyrokinetic simulations:1||Linear simulation:1||Microwave imaging reflectometers:1||ACHIEVEMENTS:1||INTERNATIONALSTELLARATORDATABASE:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||Reactive species:1||Relaxation channels:1||PHYSICS:1||RADIATION:1||

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