ScholarWorks@Korea University: Kim, Jun seok

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Kim, Jun seok (김준석)

College of Science (Department of Mathematics)

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Tel 02-3290-3077
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AllenCahn equation:43||CahnHilliard equation:38||Finite difference method:27||Multigrid method:20||Phasefield model:19||NavierStokes equation:17||finite difference method:15||Energy stability:11||BlackScholes equation:10||Phase separation:10||Operator splitting method:9||Projection method:9||Monte Carlo simulation:9||operator splitting method:8||Conservative AllenCahn equation:8||Secondorder accuracy:8||multigrid method:7||LaplaceBeltrami operator:7||Nonlinear multigrid method:7||phasefield model:7||Narrow band domain:7||Operator splitting:7||Classification:6||Equitylinked securities:6||Volume reconstruction:6||Option pricing:6||Phasefield method:6||COVID19:6||Immersed boundary method:6||Unconditionally stable scheme:6||phasefield method:6||Adaptive mesh refinement:6||Phasefield:5||Closest point method:5||BlackScholes equations:5||Fourierspectral method:5||Shape transformation:5||Unconditional energy stability:5||Finite difference:5||RayleighTaylor instability:5||Fourier spectral method:5||Curved surfaces:4||Diblock copolymer:4||option pricing:4||conservative AllenCahn equation:4||Motion by mean curvature:4||Triangular surface mesh:4||Mass conservation:4||immersed boundary method:4||Unconditional stability:4||Image segmentation:4||Hurst exponent:4||SVM:4||Multigrid:4||Phase field method:4||Pattern formation:4||Complex domain:4||Crystal growth:4||MFDFA:4||Turing pattern:3||Energy dissipation law:3||Unconditionally energystable:3||Fourthorder compact scheme:3||Image inpainting:3||Phasefield crystal equation:3||Nonlocal CahnHilliard equation:3||Cahn–Hilliard equation:3||CahnHilliard:3||unconditionally stable scheme:3||diblock copolymer:3||logarithmic free energy:3||Nonlinear multigrid:3||Coffeering effect:3||nonlocal CahnHilliard equation:3||Interfacial tension:3||projection method:3||Energy dissipation:3||Phase transition:3||phase separation:3||finite difference:3||Finite difference scheme:3||Ternary CahnHilliard system:3||Contact angle:3||Leastsquares fitting:3||Multifractality:3||Unconditionally stable:3||Unconditionally gradient stable scheme:3||Brownian bridge:3||Adaptive grid:2||Fluid flows:2||effective time step:2||Ternary CahnHilliard:2||Parallel computing:2||Phasefield simulation:2||SwiftHohenberg equation:2||Twophase fluid flow:2||Nonuniform grid:2||level set method:2||Thin film:2||Diffusion:2||Adaptive finite difference scheme:2||Phasefield surfactant:2||3D printing:2||Fourier analysis:2||SIR model:2||CrankNicolson:2||multigrid:2||ChanVese model:2||image segmentation:2||Triply periodic minimal surfaces:2||Unconditionally energy stability:2||Phasefield modeling:2||Linear multigrid:2||Evolving surface:2||Multifractal:2||Arbitrary domains:2||Boundary condition:2||Unconditionally gradient stable:2||Unsigned distance function:2||nonlinear multigrid method:2||MFDXA:2||Date assimilation:2||Scalar auxiliary variable:2||Second order accuracy:2||Reactiondiffusion system:2||secondorder accuracy:2||Dendritic growth:2||Cleavage furrow:2||surface tension:2||Spherical surface:2||Stable numerical method:2||Linear method:2||financial incentives:2||LengyelEpstein model:2||Cytokinesis:2||Lagrange multiplier:2||New Lagrange multiplier approach:2||Pinning boundary condition:2||Black–Scholes equations:2||NavierStokes equations:2||LandauLifshitz equation:2||adaptive mesh refinement:2||Degenerate mobility:2||ECG:2||ModicaMortola functional:2||Unconditionally energy stable:2||code implementations:2||Energy minimization:2||Multicomponent fluid flows:2||Efficient algorithm:2||unconditionally gradient stable scheme:2||Improved SAV approach:1||Metamorphosis:1||dendritic pattern formation:1||Agricultural futures:1||Rhinitis:1||Bacterial Foodborne Diseases:1||Brownian bridge technique:1||mass correction scheme:1||Multicomponent:1||MCS:1||Adaptive numerical method:1||Fastest growing mode:1||l(0) gradient minimization:1||Conservative discretization:1||Iterative methods:1||Moving overset grid:1||Multicomponent CahnHilliard system:1||Curved surface:1||Nonuniform grid:1||Kinetic parameters:1||fluid vesicles:1||hybrid method:1||implicit finite difference method:1||derivative securities:1||nonuniform grid.:1||multidimensional BlackScholes equations:1||Compound droplet:1||CrankNicolson scheme:1||Pseudospectral method:1||Greek:1||twoasset option:1||Reactiondiffusion model:1||Buoyancydriven mixing:1||OSM:1||LeeSeo model:1||multicomponent:1||Cell mobility:1||Marangoni stress:1||ModicaMortola:1||multiphase flow:1||Pinchoff:1||Continuum surface tension:1||Multicomponent CahnHilliard equation:1||hybrid numerical method:1||Ternary Cahn&#8211:1||Brownian dynamics:1||homopolymer mixtures:1||FDM:1||Stabilization technique:1||interfacial function:1||Swift–Hohenberg equation:1||Arbitrarydomains:1||Secondorderscheme:1||simple shear flow:1||Artificial curvature effect:1||Multicomponent flow:1||Fully explicit scheme:1||Multigrid algorithm:1||Energy stable schemes:1||TFOV:1||illposed problem:1||augmented Lagrangian method:1||PhasefieldDNN:1||Solidstate sintering:1||diffusion equation:1||Cahn equation:1||Isotropic Discretization:1||Multiple physical field coupling:1||Cubic surface:1||GrayScott:1||the CahnHilliard (CH) equation:1||Landau–Lifshitz–Gilbert equation:1||Magnetization dynamics:1||Heat sinks:1||Continuous volatility:1||Discrete cosine transform:1||Shellinfill structures:1||Multiscale topology optimization:1||NavierStokesCahnHilliard equations:1||Timedependent SUC model:1||Taylor dispersion:1||Unique solvability:1||KevinHelmholtz instability:1||Periodic travelling waves:1||phasefield equations:1||Multifractaity:1||Incompressible NavierStokes equation:1||Network:1||planar visualizations:1||Crosscorrelation:1||closest point method:1||Cross section interpolating:1||Solidification:1||Flow on a fibre:1||Benchmark problem:1||fast Fourier transform:1||Adaptive timestepping:1||MERSCoV:1||Implicit:1||Surface remeshing algorithm:1||pathaveraged option value.:1||Tumor growth:1||Soft Matter: Polymers and Polyelectrolytes:1||contact angle condition:1||Hexcylinder phase:1||Coupled chemotaxisfluid model:1||Bioconvection:1||elastic inhomogeneity:1||jumpdiffusion:1||Diffuse interface model:1||Navier–Stokes equation:1||BlackScholes partial differential equation:1||extrapolation:1||MumfordShah functional:1||finitedifference method:1||Absorbing nonreflecting boundary treatment:1||Articular cartilage regeneration:1||Inclined channel:1||Linearly stabilized splitting scheme:1||Firstorder reaction network:1||Monte Carlo method:1||interface capturing:1||semiimplicit scheme:1||Smooth Curve(매끄러운 곡선):1||Fund:1||SSEC:1||CahnHilliardDarcy system:1||OhtaKawasaki model:1||Conservative SwiftHohenberg model:1||Efficient methods:1||Twophase flows:1||Topology optimization:1||2D MFDFN:1||Norm:1||Novel SAV approach:1||Phase field vesicle model:1||Crystallization:1||Chaotic sequence:1||phasefield method.:1||Timedependent evaporation rate:1||calibration:1||Thermalfluid topology optimization:1||linear convex splitting:1||Voxelization:1||3D curved surfaces:1||Contact angle condition:1||Multi phase system:1||Harvesting term:1||Allen:1||Diffusion equation:1||Fast Monte Carlo method:1||Timedependent volatility:1||Numerical design procedure:1||Implicit surfaces:1||LifshitzPetrich model:1||alveolar/venous blood:1||diffusion:1||Melt pool:1||Phase exchange:1||New SSAV approach:1||logistic source:1||tumor growth application:1||leastsquares fitting:1||Nonstandard variable mobility:1||kNN:1||Retina:1||image processing:1||Image smoothing:1||narrow band domain:1||Mobile platform:1||Greeks:1||Explicit hybrid method:1||Vectorvalued AllenCahn equation:1||Zebra pattern formation:1||Optimization:1||Benzene:1||Volume correction algorithm:1||Hybrid explicit scheme:1||nonuniform grid:1||Continuum surface force:1||high correlation:1||Practically stable scheme:1||Volatility smile:1||wall effect:1||Firstorder partial differential equation:1||Dirichlet boundary condition:1||Practically unconditionally gradient stable:1||Crank–Nicolson scheme:1||Level set model:1||Variable density model:1||regularized Dirac delta function:1||area preserving:1||Turing instability:1||nonlinear diffusion equation:1||Constant mean curvature:1||Decoupled scheme:1||ice melting:1||Energy stable scheme:1||Black–Scholes equation:1||modified AllenCahn equation:1||level set function:1||Fully decoupled scheme:1||Nevus:1||melanoma:1||Twophase thermodynamic flow:1||Convex splitting scheme:1||Maximum principle preserving:1||cumulative summation:1||Incompressible fluid flows:1||option price:1||Crystal growth model:1||Energy stable method:1||discrete Laplace operator:1||Twophase flow:1||Computer simulation:1||Binary surfactant model:1||Surfactantladen phase separation:1||Higuchi's Hurst Exponent:1||fourthorder accurate compact method:1||explicit Euler method:1||Triply periodic minimal surface:1||Timedependent interest rate:1||Volume merging algorithm:1||Variable viscosity:1||Connected region:1||Extending domain:1||Multiple intense zebra stripe formation:1||Boundary wall:1||Mesh sizedependent parameter:1||Modified CahnHilliard equation:1||Triangle surface mesh:1||explicit hybrid method:1||graph drawing:1||CrossCorrelation:1||Meteorological Factors:1||Modified NaiverStokes equation:1||Antibubble:1||ELS:1||surface reconstruction:1||Gaussian filter:1||Linear stability analysis:1||Rayleigh instability:1||Navier Stokes equation:1||Cavity flow:1||Tissue growth:1||spectral method:1||Ohta Kawasaki model:1||BlackScholes partial differential equation:1||Explicit:1||European options:1||continuum surface force:1||Navier–Stokes equation.:1||Offset surface reconstruction:1||periodic traveling waves:1||log transformation:1||equitylinked securities:1||Drop deformation:1||Finite element method:1||Semiimplicit finite difference method:1||Multiphase flow:1||biCGSTAB:1||volume conserving:1||Selfsimilar solution:1||Linear geometric multigrid:1||interface dynamics:1||ratiodependent predatorprey:1||Velocity (속도):1||snow crystal growth:1||Liquid jet:1||Local volatility:1||MFDMCCA:1||Saul'yevtype:1||FloryHuggins potential:1||Fingerprint restoration:1||Phasefield surfactant fluid system:1||Saul'yevtype method:1||SAV approach:1||CHmodel:1||Phasefield methods:1||Image encryption:1||solar energy:1||optimal orientation:1||mathematical modeling:1||Cellcentered finite difference method:1||Mobile platform.:1||Spacetime dependent Lagrange multiplier:1||Secondorder accurate:1||Hyperbolic tangent property:1||Lattice Boltzmann method:1||MRIs:1||Binary fluid system:1||Arbitrary domain:1||Diffuse interface model:1||Weakly nonlinear analysis:1||3D mesh denoising:1||Image inpanting:1||PSNR:1||Ferromagnetism:1||Shape and performance control:1||Colloidal crystal model:1||Porous infill architecture:1||stability analysis:1||numerical method:1||Chemical reactions on:1||normalized timefractional diffusion ff usion equation:1||Droplet evaporation:1||Decoupled schemes:1||Backward differentiation formula:1||spacetime dependent Lagrange multiplier:1||operator splitting:1||Least square support vector machine:1||superfast computation:1||Conservative scheme:1||convex splitting:1||Far field boundary conditions:1||Adaptive timestepping method:1||blockcopolymer:1||Practically unconditionally gradient stable scheme:1||Contractile elastic ring:1||local defectivity control:1||ternary fluid flows:1||Dirichlet boundary:1||landscape features:1||Simpson's rule:1||KelvinHelmholtz instability:1||Linear growth rate:1||Shear flow:1||Surfactant:1||twophase flows:1||Phase change:1||shear flow:1||Characteristic method:1||Ncomponent CahnHilliard system:1||Vectorvalued Allen Cahn equations:1||twophase fluid flow:1||Cell growth:1||fingering instability:1||phasefield:1||Hurst Exponent:1||SUC model:1||Alternating direction explicit scheme:1||Highorder polynomial free energy:1||Implicitexplicit RK scheme:1||Tissue engineering scaffolds:1||MSAV approach:1||Explicit finite difference method:1||Energydissipationlaw:1||Stokes equation:1||local volatility function:1||Multiplicative cascade images:1||Ice crystal growth:1||Linearly decoupled scheme:1||Incompressible flows:1||Scrambling:1||3D volume reconstruction:1||SwiftHohenberg model:1||image segmenta tion:1||Stripe formation:1||Phase field crystal model:1||Linearly consistent method:1||volatility:1||Nonhomogeneous zebra pattern formation:1||Relaxation technique:1||? t:1||Multiplicative cascades:1||Fast evolution scheme:1||3D MFDFA:1||Persistence:1||Multicomponent vesicles:1||alternating direction explicit method:1||Singularity:1||Surface lattice Boltzmann method:1||Fluidsurfactant system:1||gas exchange:1||inert gas:1||COVID19 pandemic:1||Logarithmic potential:1||Modified AllenCahn equation:1||Optimal nonuniform grid:1||Polynomial free energy:1||Epidemic model:1||Landscape features:1||Brain MRI Image:1||equilibrium solution:1||PM10:1||Bronchitis:1||Crystal morphology:1||Unorganized points:1||Point cloud:1||ternary CahnHilliard system:1||markerandcell mesh:1||Growth kinetics:1||Phenol:1||Twophase fluid:1||numerical periodicity:1||motion by mean curvature:1||Multiphase flows:1||multigrid method.:1||image inpainting:1||explicit finite difference method:1||linear boundary condition:1||Lamellar phase:1||Wavelength:1||adaptive grid:1||Free surface waves:1||Regimeswitching model:1||Chemical processes:1||Mathematical modeling:1||cashornothing:1||droplet deformation:1||Finitedifference method.:1||option pricing.:1||Boussinesq approximation model:1||indicator function:1||Numerical simulation:1||Parameter(매개변수):1||nonlinear multigrid:1||generalized Hurst exponent:1||Ternary CahnHilliard fluids:1||Volume merging method:1||Conservative finite difference method:1||Corrected energy:1||Effective time step:1||Phasefield crystal model:1||Spinodal decomposition:1||EquityLinked Securities:1||Fluidstructure interaction:1||highorder polynomial free energy:1||Phase field model:1||Threecomponent fluids:1||image deblurring:1||DNN:1||triangular meshes:1||automatic fingerprint restoration:1||Stable timestepping scheme:1||Porous scaffolds:1||Nucleation:1||Time varying SUC model:1||Distance function:1||Systems of CahnHilliard equations:1||Crosscorrelations:1||tissue growth:1||boundary condition:1||Growth from melt:1||nonlinear convex splitting scheme:1||Honeycomb:1||Surface reconstruction:1||l(0) sparsity:1||Spacetimedependent Lagrange multiplier:1||unconditionally gradient stability:1||incompressible NavierStokes equations:1||Optimal parameter fitting:1||Microbial growth:1||Logarithmic free energy:1||Conservation of mass:1||Oxytactic bacteria:1||Surface tension and buoyancy effects:1||Billowing cloud formation:1||finite difference method.:1||Peclet condition:1||Micromagnetics simulations:1||computational fluid dynamics:1||Nonlinear diffusion equations:1||Hydrogel:1||ADI:1||Grain growth:1||phase field model:1||Wulff construction:1||thin film:1||triangular surface mesh:1||PDE on surface:1||Efficient SMSAV approach:1||MFDMA:1||Copolymer:1||CahnHilliard system:1||Linear convex splitting:1||Nonlinear curvefit:1||Gradient flows:1||STSAV approach:1||Structurepreserving model:1||Diblock copolymer melts:1||MFDCCA:1||twophase flow:1||solar panel:1||hurst exponent:1||interest rate:1||Dissipation law:1||Fatality rate:1||Conservative AllenCahn model:1||constrained problem:1||AllenCahn:1||Predatorprey model:1||Consistently energystable method:1||maximum principle:1||Numerical algorithm:1||Lagrange multiplier approach:1||Kolmogorov Complexity:1||Shannon Entropy:1||Novel phasefield model:1||Quasicrystals:1||partial pressure:1||respiratory system:1||Explicit Euler method:1||Stability analysis:1||Selective laser melting:1||Diffuseinterface model:1||Triangular mesh:1||Modified phasefield surfactant:1||CahnHilliardHeleShaw:1||Side wall boundary:1||SUC epidemic model:1||porous surface:1||2D MFDFA:1||nonlocal AllenCahn equation:1||crystal growth:1||Crude oil:1||Closestpoint method:1||porous structure:1||Explicit numerical method:1||Ncomponent CahnHilliard equation:1||bioscaffold:1||triply periodic minimal surface:1||Hexagonal pattern:1||optimal splitting parameter:1||solvability:1||Inflowoutflow boundary condition:1||Explicit Euler's method:1||Modeling:1||predatorprey model:1||penalty method:1||linear interpolation:1||Allen Cahn equation:1||viscous CahnHilliard equation:1||farfield boundary conditions:1||Forced Kortewegde Vries equation:1||Numerical analysis:1||remeshing:1||Timedependent pressure boundary condition:1||Volumepreserving:1||Comparison study:1||Axisymmetric simulation:1||Multiple crystals growth:1||NavierStokes:1||Scaffolds:1||Allen–Cahn equation:1||Ncomponent CahnHilliard:1||Hilliard model:1||Binary data classification:1||MFXDMA:1||Optimal parameter estimation:1||Second order:1||Highorder schemes:1||Local volatility surface:1||Axisymmetric compound liquid threads:1||Implicit method:1||Stable scheme:1||Lagrange multiplier method:1||Square PFC model:1||3D surfaces:1||LSSE:1||droplet breakup:1||CahnHilliard model:1||Anisotropy:1||Orientational field model:1||Threephase conservative allenCahn fluids:1||policymakers:1||Local fitting:1||Finite volume scheme:1||Twophase surfactant system:1||Compound droplets:1||Finite Difference Method:1||Discrete Laplacian Operator:1||Isotropic Stencil:1||Heat convection:1||di ff usion equation:1||Multifractal Features:1||Formal secondorder accuracy:1||Energy structure:1||Modified Allen–Cahn equation:1||MATLAB code:1||Unconditionally stability:1||normalized timefractional SIR equation:1||epidemic mathematical model:1||3D reconstruction:1||Periodic drug delivery:1||Gamma function:1||Point clouds:1||

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