A method for incorporating Gauss' lasw into electromagnetic pic codes
Journal of Computational Physics
Journal of Computational Physics
Finite difference schemes and partial differential equations
Finite difference schemes and partial differential equations
On a finite-element method for solving the three-dimensional Maxwell equations
Journal of Computational Physics
A splitting algorithm for Vlasov simulation with filamentation filtration
Journal of Computational Physics
The origin of spurious solutions in computational electromagnetics
Journal of Computational Physics
Conservative numerical schemes for the Vlasov equation
Journal of Computational Physics
Outflow Boundary Conditions for the Fourier Transformed One-Dimensional Vlasov–Poisson System
Journal of Scientific Computing
Plasma Physics Via Computer
A numerical scheme for the integration of the Vlasov--Maxwell system of equations
Journal of Computational Physics
Outflow boundary conditions for the Fourier transformed two-dimensional Vlasov equation
Journal of Computational Physics
Outflow boundary conditions for the Fourier transformed three-dimensional Vlasov-Maxwell system
Journal of Computational Physics
Parallelization of a Vlasov-Maxwell solver in four-dimensional phase space
Parallel Computing
Scalable Direct Vlasov Solver with Discontinuous Galerkin Method on Unstructured Mesh
SIAM Journal on Scientific Computing
Energy-conserving discontinuous Galerkin methods for the Vlasov-Ampère system
Journal of Computational Physics
Hi-index | 31.46 |
The two-dimensional Vlasov-Maxwell system, for a plasma with mobile, magnetised electrons and ions, is investigated numerically. A previously developed method for solving the two-dimensional electrostatic Vlasov equation, Fourier transformed in velocity space, for mobile electrons and with ions fixed in space, is generalised to the fully electromagnetic, two-dimensional Vlasov-Maxwell system for mobile electrons and ions. Special attention is paid to the conservation of the divergences of the electric and magnetic fields in the Maxwell equations. The Maxwell equations are rewritten, by means of the Lorentz potentials, in a form which conserves these divergences. Linear phenomena are investigated numerically and compared with theory and with previous numerical results.