Neoclassical transport simulation code (FORTEC-3D) applicable to non-axisymmetric configurations is developed. A new hybrid simulation model in which ion transport is solved by using the δ f Monte-Carlo method including the finite-orbit-width effects, while electron transport is solved by a reduced ripple-averaged kinetic equation, is adopted. This model makes it possible to simulate the dynamism of non-local transport phenomena with a self-consistently developing radial electric field within an allowable computation time. Time evolution of a radial electric field in LHD plasma is simulated in the full volume of the confinement region, and the finiteorbit- width effect of neoclassical transport is found to make the negative ambipolar electr...
The radial electric field Er at the tokamak plasma edge is simulated both with a two-dimensional (2D...
Abstract. The neoclassical return current and parallel viscosity due to the radial electric field (n...
The stellarator neoclassical transport due to particles trapped in local helical wells is calculated...
Neoclassical transport simulation code (FORTEC-3D) applicable to non-axisymmetric configurations is ...
The progress in a 3-dimensional, non-local neoclassical transport simulation code “FORTEC-3D” is des...
A Monte Carlo neoclassical transport code has been developed to solve for the equilibrium ambi-polar...
A 5D Monte Carlo particle simulation method for advancing rotating plasmas in tori is presented. The...
Drift kinetic and gyrokinetic theories and simulations are powerful means for quantitative predictio...
Neoclassical transport analyses have been performed for a high electron temperature LHD plasma with ...
An impurity hole observed in the large helical device (LHD) is a hollow density profile of an impuri...
Neoclassical transport coefficients are computed in LHD configurations with two different values of ...
The magnitude of the radial electric field (Er), resulting from nonambipolar fluxes of neoclassical ...
Neoclassical transport simulation using the δ f Monte-Carlo method is carried out to investigate the...
Improving confinement of the particle and energy transport is an importan...
"Effects of finite-beta and radial electric fields on the neoclassical transport in the Large Helica...
The radial electric field Er at the tokamak plasma edge is simulated both with a two-dimensional (2D...
Abstract. The neoclassical return current and parallel viscosity due to the radial electric field (n...
The stellarator neoclassical transport due to particles trapped in local helical wells is calculated...
Neoclassical transport simulation code (FORTEC-3D) applicable to non-axisymmetric configurations is ...
The progress in a 3-dimensional, non-local neoclassical transport simulation code “FORTEC-3D” is des...
A Monte Carlo neoclassical transport code has been developed to solve for the equilibrium ambi-polar...
A 5D Monte Carlo particle simulation method for advancing rotating plasmas in tori is presented. The...
Drift kinetic and gyrokinetic theories and simulations are powerful means for quantitative predictio...
Neoclassical transport analyses have been performed for a high electron temperature LHD plasma with ...
An impurity hole observed in the large helical device (LHD) is a hollow density profile of an impuri...
Neoclassical transport coefficients are computed in LHD configurations with two different values of ...
The magnitude of the radial electric field (Er), resulting from nonambipolar fluxes of neoclassical ...
Neoclassical transport simulation using the δ f Monte-Carlo method is carried out to investigate the...
Improving confinement of the particle and energy transport is an importan...
"Effects of finite-beta and radial electric fields on the neoclassical transport in the Large Helica...
The radial electric field Er at the tokamak plasma edge is simulated both with a two-dimensional (2D...
Abstract. The neoclassical return current and parallel viscosity due to the radial electric field (n...
The stellarator neoclassical transport due to particles trapped in local helical wells is calculated...