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RYU, CHANG MO(유창모)

Department: Dept of Physics(물리학과)

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PLASMA:7||ADHESION:4||TRANSPORT:4||POLYMERS:4||DYNAMICS:4||MECHANISM:4||MODEL:4||SYSTEMS:4||STATES:4||TURBULENCE:3||SIMULATION:3||plasma:3||LOOPS:3||INSTABILITY:3||SPIN:3||SPECTRA:3||MODES:3||THIN CURRENT SHEETS:3||XPS:3||TOKAMAK:3||GENERATION:3||SOLARWIND:3||GLOWDISCHARGE:2||EQUATIONS:2||PARTICLES:2||TWOFOLDDEGENERATE BAND:2||SOLAR ATMOSPHERE:2||aging:2||SHEATH:2||ZONAL FLOWS:2||BICOHERENCE:2||SUBSTORM ONSET:2||BERRY PHASE:2||FLOW:2||SEARCH:2||PLASMA INSTABILITIES:2||TEMPERATURE:2||crystallinity:2||ENERGY:2||INTERCHANGE MODES:2||FLUX TUBES:2||NEUTRAL PARTICLES:2||photonassisted tunneling:2||SCATTERING:2||oxygen:2||TAIL:2||BALLOONING INSTABILITY:2||ELECTROMAGNETICRADIATION:2||TIME:2||FILMS:2||crosslinking:2||SPACE PLASMAS:2||argon:2||Electron beamplasma instability:2||INTERPLANETARY SPACE:2||STABILIZATION:2||SINGLE:2||HARMONIC LANGMUIRWAVES:2||STABILITY:2||JUNCTIONS:2||HIGHINTENSITY LASERS:1||FINITEAMPLITUDE:1||IONS:1||QUANTUMFIELD THEORY:1||superconductor:1||quasiparticle transport:1||DISCRETE ELECTRONIC STATES:1||microwave:1||BEHAVIOR:1||FLUX:1||dwave superconductor:1||QUANTUMMECHANICS:1||energetic particle:1||NONLINEARINTERACTION:1||ELECTRONBEAMS:1||STRANGE ATTRACTORS:1||PROFILE:1||CODE:1||STOCHASTIC ACCELERATION:1||Laserplasma interaction:1||Self focusing harmonic generation density ripple plasma:1||Particleincell simulation:1||TREATED SILICONERUBBER:1||HYDROPHOBIC RECOVERY:1||CRITERION:1||EIGENMODES:1||EXCITATION:1||ELECTRON ACCELERATION:1||PERTURBATIVE EXPANSION:1||OPTIMIZED EXPANSION:1||SUPERCONDUCTIVITY:1||nonequilibrium Green&apos:1||quantum dot:1||SINGLEELECTRON TRANSISTOR:1||electrical resistivity:1||RFTF:1||MESOSCOPIC RINGS:1||CURRENT MAGNIFICATION:1||RESONANTLY COUPLED CAVITIES:1||NORMALMETAL RINGS:1||VOLTAGE:1||KINK INSTABILITY:1||MAGNETOTAIL:1||DISRUPTION:1||DISPERSION FUNCTION:1||Cluster plasma:1||LASER:1||EMISSION:1||FREQUENCY:1||capacitively coupled plasma:1||PLASMAS:1||HELIUM:1||BOUNDARY:1||KAPPADISTRIBUTIONS:1||MAGNETICFIELD:1||CATHODEDISCHARGE:1||DEVICES:1||INSTABILITIES:1||RENORMALIZATION:1||tunneling current:1||PHASE:1||LOOP:1||TRANSMISSION:1||weak turbulence:1||RF DISCHARGES:1||RF FIELD:1||LANGMUIRWAVES:1||bispectral analysis:1||COHERENT:1||correlation dimension:1||edge turbulence:1||EARTHS MAGNETOSPHERE:1||Ideal MHD stability:1||BEAMPLASMA INTERACTION:1||GAS:1||Capacitivelycoupled plasma:1||Magnetic field:1||SURFACE MODIFICATION:1||PRESSURE:1||PULSE:1||ABSORPTION:1||HYDROMAGNETICWAVES:1||DECAY INSTABILITY:1||EVOLUTION:1||ATMOSPHERICPRESSURE:1||GAUSSIAN APPROXIMATION:1||s function:1||ICP:1||PERSISTENT CURRENTS:1||QUANTUM TRANSPORT:1||ELECTRONS:1||CORONAL LOOPS:1||MASSIVE GAUGETHEORIES:1||WAVEGUIDES:1||SOLAR RADIOBURSTS:1||plasma turbulence:1||FLUCTUATIONS:1||PARTICLE SIMULATIONS:1||NONLINEAR EVOLUTION:1||IONCYCLOTRON:1||BURSTS:1||particleincell simulation:1||RF DISCHARGE:1||CONTACTANGLE:1||POLYPROPYLENE:1||SATURNS MAGNETOSPHERE:1||JET:1||Electromagnetic sideband waves:1||UNDERDENSE PLASMAS:1||MODULATIONAL INSTABILITY:1||SIMULATIONS:1||coulomb blockade:1||SYSTEM:1||LEADS:1||IONCYCLOTRON FREQUENCY:1||SMALL COLD BEAM:1||zonal flow:1||HYBRID DRIFT INSTABILITY:1||CURRENT DISRUPTION:1||ENERGYSPECTRA:1||WAVES:1||PARAMETRICINSTABILITIES:1||DRIVEN:1||SPECTRUM:1||dualfrequency:1||magnetic field:1||atmosphericpressure glow discharge (APGD):1||AIR:1||ION KINETICS:1||CORONA:1||DRIFTWAVE TURBULENCE:1||COUPLEDCLUSTER METHOD:1||BCS SUPERCONDUCTIVITY:1||STATISTICS:1||QUANTUM:1||OSCILLATIONS:1||ION ENERGYDISTRIBUTION:1||DYNAMOS:1||WAVE:1||mirror plasma:1||EARTHS MAGNETOTAIL:1||Plasma simulation:1||ELECTROMAGNETIC EMISSION:1||Generalized weak turbulence theory:1||kinetic simulation:1||microplasma:1||HDPE:1||angleresolved XPS:1||SURFACE:1||oxygenplasma:1||ABSORPTION SPECTROSCOPY NEXAFS:1||SURFACEANALYSIS:1||AMORPHOUS FERROMAGNETS:1||TOKAMAKS:1||Stimulated Raman forward scattering:1||NONSTANDARD EXPANSION TECHNIQUES:1||superconductivity:1||REGIME:1||FRACTIONAL STATISTICS:1||BALLISTICTRANSPORT:1||H/E:1||REVERSED CONFIGURATIONS:1||DISCHARGES:1||dusty plasma:1||dust ion acoustic solitary wave:1||DOUBLELAYERS:1||MAGNETIC NEUTRAL SHEET:1||KSTAR:1||PLASMA SHEET:1||PRESSURE RF DISCHARGE:1||microdischarge:1||DISCHARGE:1||CORONA DISCHARGE:1||WATER:1||highdensity polyethylene:1||surface rearrangement:1||Prelaser pulses:1||BEAM:1||ACCELERATION:1||RESONANCE:1||Hanbit:1||ALLOYS:1||INTERFERENCE:1||radiations in plasmas:1||HEATINGMODE TRANSITION:1||PINCH:1||beam plasma interaction:1||Langmuir turbulence:1||TURBULENCE THEORY:1||ANOMALOUS RESISTIVITY:1||III RADIOBURSTS:1||Raman instability:1||INTENSE LASER:1||Plasma emission:1||AMPLIFICATION:1||Dualfrequency:1||TRANSITION:1||PARTICLE:1||LDPE:1||THERMOPOWER:1||

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