sll_m_time_propagator_pic_vm_3d3v_cef.F90 File Reference

#include "sll_assert.h"
#include "sll_errors.h"
#include "sll_memory.h"
#include "sll_working_precision.h"

Include dependency graph for sll_m_time_propagator_pic_vm_3d3v_cef.F90:

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Data Types
type	sll_t_time_propagator_pic_vm_3d3v_cef
	Hamiltonian splitting type for Vlasov-Maxwell 3d3v. More...

Modules
module	sll_m_time_propagator_pic_vm_3d3v_cef
	Particle pusher based on Hamiltonian splitting using in Crouseilles, Einkemmer, Faou for 3d3v Vlasov-Maxwell.

Functions/Subroutines
subroutine	strang_splitting_pic_vm_3d3v (self, dt, number_steps)
	Finalization. More...
subroutine	lie_splitting_pic_vm_3d3v (self, dt, number_steps)
	Lie splitting. More...
subroutine	lie_splitting_back_pic_vm_3d3v (self, dt, number_steps)
	Lie splitting (oposite ordering) More...
subroutine	operatorhp_pic_vm_3d3v (self, dt)
	Push H_p: Equations to be solved $X^{n+1}=X^n+\Delta t V^n$ $M_1 e^n= M_1 e^n- \int_{t^n}^{t^{n+1}} \mathbb{\Lambda}^1(X(\tau))^\top d\tau \mathbb{W}_q V^n$. More...
subroutine	compute_particle_boundary (self, xold, xnew, vi, wi)
	Helper function for operatorHp. More...
subroutine	operatorhb_pic_vm_3d3v (self, dt)
	Push H_B: Equations to be solved $(\mathbb{I}-\Delta \frac{\Delta t q}{2 m} \mathbb{B}(X^n,b^n) V^{n+1}=(\mathbb{I}+ \frac{\Delta t q}{2 m} \mathbb{B}(X^n,b^n) ) V^n$ $M_1 e^{n+1}=M_1 e^n+\Delta t C^\top M_2 b^n$. More...
subroutine	operatorhe_pic_vm_3d3v (self, dt)
	Push H_E: Equations to be solved $V^{n+1}=V^n+\Delta t\mathbb{W}_{\frac{q}{m}} \mathbb{Lambda}^1(X^n) e^n$ $b^{n+1}=b^n-\Delta t C e^n$. More...
subroutine	initialize_pic_vm_3d3v (self, maxwell_solver, particle_mesh_coupling, particle_group, phi_dofs, efield_dofs, bfield_dofs, x_min, Lx, boundary_particles, betar, electrostatic, rhob, control_variate)
	Constructor. More...
subroutine	delete_pic_vm_3d3v (self)
	Destructor. More...