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KWON, YONGHOON (권용훈)

Dept of Mathematics(수학과)

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parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||parameter estimation:5||EQUATION:4||MODEL:4||infiltration:3||BURGERSEQUATION:3||NUMERICAL INVERSION:2||spectral approximation:2||approximation:2||MASSTRANSPORT:2||APPROXIMATION:2||GROUNDWATER:2||s operator:2||Green&apos:2||Burgers equation:2||INVERSE PROBLEM:2||BlackScholes equation:2||discontinuous conductivity:1||timeintegration:1||PARAMETERESTIMATION:1||The closed form reproducing polynomial particle (RPP) shape functions:1||Reproducing kernel particle (RKP) shape functions:1||NODE METHOD:1||direct method:1||optimal exercise curve:1||NUMERICAL IDENTIFICATION:1||SHAPE FUNCTIONS:1||SINGULARITIES:1||PARTITION:1||UNITY:1||identifiability under approximation:1||observation design:1||CONSTANT:1||FINITEELEMENT METHOD:1||LAPLACE TRANSFORM GALERKIN:1||convergence analysis:1||s function:1||ELLIPTICEQUATIONS:1||Inverse Laplace transform:1||quasilinear convectiondiffusion equation:1||numerical result:1||inverse Laplace transform:1||GALERKIN:1||FREEBOUNDARY:1||EQUATIONS:1||Stokes problem:1||American option:1||ChebyshevLegendre approximations:1||COEFFICIENT:1||FINITEELEMENT SOLUTIONS:1||POTENTIAL PROBLEMS:1||GROWTH:1||local Green&apos:1||free boundary problem:1||POROUSMEDIA:1||Boundary element method (BEM):1||Finite difference method:1||OPTIONS:1||finiteelement method:1||porous media:1||transport equation:1||spectral accuracy:1||OPTION:1||convergence and spectral accuracy:1||parameter identification:1||spectral Galerkin method:1||FLOW:1||Stokes equations:1||CONTAMINANT TRANSPORT:1||

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