The progress in a 3-dimensional, non-local neoclassical transport simulation code “FORTEC-3D” is described. The main purpose of the code is to solve the drift-kinetic equation in general a 3-dimensional configuration using the δf Monte Carlo method, and to calculate neoclassical fluxes and the time evolution of the ambipolar radial electric field simultaneously. This article explains new numerical schemes adopted in FORTEC-3D in order to overcome numerical problems, which happen especially in the cases where the bifurcation of radial electric field occurs. Examples of test simulation for an LHD magnetic field configuration with a bifurcated electric field are also shown. With improved numerical schemes, FORTEC-3D can calculate neoclassical ...
A 5D Monte Carlo particle simulation method for advancing rotating plasmas in tori is presented. The...
A Monte Carlo neoclassical transport code has been developed to solve for the equilibrium ambi-polar...
An impurity hole observed in the large helical device (LHD) is a hollow density profile of an impuri...
Neoclassical transport simulation code (FORTEC-3D) applicable to non-axisymmetric configurations is ...
Neoclassical transport simulation code (FORTEC-3D) applicable to non-axisymmetric configurations is ...
Drift kinetic and gyrokinetic theories and simulations are powerful means for quantitative predictio...
A neoclassical transport simulation code (FORTEC-3D) applicable to threedimensional configurations h...
"In order to analyze neoclassical transport phenomena in/around a magnetic field configuration with ...
"Effects of finite-beta and radial electric fields on the neoclassical transport in the Large Helica...
Two simulation codes that solve the drift-kinetic or gyrokinetic equation in toroidal plasmas are be...
"Recent Large Helical Device experiments show that the transport modeling based only on the fluid de...
Non-axisymmetric magnetic perturbations can fundamentally change neoclassical transport in tokamaks ...
Neoclassical transport coefficients are computed in LHD configurations with two different values of ...
The linearized drift kinetic equation is solved numerically to obtain the Onsager transport matrix f...
A new code, the Neoclassical Ion-Electron Solver (NIES), has been written to solve for stationary, a...
A 5D Monte Carlo particle simulation method for advancing rotating plasmas in tori is presented. The...
A Monte Carlo neoclassical transport code has been developed to solve for the equilibrium ambi-polar...
An impurity hole observed in the large helical device (LHD) is a hollow density profile of an impuri...
Neoclassical transport simulation code (FORTEC-3D) applicable to non-axisymmetric configurations is ...
Neoclassical transport simulation code (FORTEC-3D) applicable to non-axisymmetric configurations is ...
Drift kinetic and gyrokinetic theories and simulations are powerful means for quantitative predictio...
A neoclassical transport simulation code (FORTEC-3D) applicable to threedimensional configurations h...
"In order to analyze neoclassical transport phenomena in/around a magnetic field configuration with ...
"Effects of finite-beta and radial electric fields on the neoclassical transport in the Large Helica...
Two simulation codes that solve the drift-kinetic or gyrokinetic equation in toroidal plasmas are be...
"Recent Large Helical Device experiments show that the transport modeling based only on the fluid de...
Non-axisymmetric magnetic perturbations can fundamentally change neoclassical transport in tokamaks ...
Neoclassical transport coefficients are computed in LHD configurations with two different values of ...
The linearized drift kinetic equation is solved numerically to obtain the Onsager transport matrix f...
A new code, the Neoclassical Ion-Electron Solver (NIES), has been written to solve for stationary, a...
A 5D Monte Carlo particle simulation method for advancing rotating plasmas in tori is presented. The...
A Monte Carlo neoclassical transport code has been developed to solve for the equilibrium ambi-polar...
An impurity hole observed in the large helical device (LHD) is a hollow density profile of an impuri...