sll_m_time_propagator_pic_vm_1d2v_hs_trafo.F90 File Reference

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

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Data Types
type	sll_t_time_propagator_pic_vm_1d2v_hs_trafo
	Hamiltonian splitting type for Vlasov-Maxwell 1d2v. More...

Modules
module	sll_m_time_propagator_pic_vm_1d2v_hs_trafo
	Particle pusher based on Hamiltonian splitting for 1d2v Vlasov-Maxwell with coordinate transformation.

Functions/Subroutines
subroutine	strang_splitting_pic_vm_1d2v (self, dt, number_steps)
	Finalization. More...
subroutine	lie_splitting_pic_vm_1d2v (self, dt, number_steps)
	Lie splitting. More...
subroutine	lie_splitting_back_pic_vm_1d2v (self, dt, number_steps)
	Lie splitting (oposite ordering) More...
subroutine	operatorhp_pic_vm_1d2v (self, dt)
	Push Hp1: Equations to solve are \partial_t f + v_1 \partial_{x_1} f = 0 -> X_new = X_old + dt V_1 V_new,2 = V_old,2 + \int_0 h V_old,1 B_old \partial_t E_1 = - \int v_1 f(t,x_1, v) dv -> E_{1,new} = E_{1,old} - \int \int v_1 f(t,x_1+s v_1,v) dv ds \partial_t E_2 = 0 -> E_{2,new} = E_{2,old} \partial_t B = 0 => B_new = B_old. More...
subroutine	operatorhe_pic_vm_1d2v (self, dt)
	Push H_E: Equations to be solved \partial_t f + E_1 \partial_{v_1} f + E_2 \partial_{v_2} f = 0 -> V_new = V_old + dt * E \partial_t E_1 = 0 -> E_{1,new} = E_{1,old} \partial_t E_2 = 0 -> E_{2,new} = E_{2,old} \partial_t B + \partial_{x_1} E_2 = 0 => B_new = B_old - dt \partial_{x_1} E_2. More...
subroutine	operatorhb_pic_vm_1d2v (self, dt)
	Push H_B: Equations to be solved V_new = V_old \partial_t E_1 = 0 -> E_{1,new} = E_{1,old} \partial_t E_2 = - \partial_{x_1} B -> E_{2,new} = E_{2,old}-dt*\partial_{x_1} B \partial_t B = 0 -> B_new = B_old. More...
subroutine	initialize_pic_vm_1d2v (self, maxwell_solver, kernel_smoother_0, kernel_smoother_1, particle_group, efield_dofs, bfield_dofs, x_min, Lx, map, electrostatic)
	Constructor. More...
subroutine	delete_pic_vm_1d2v (self)
	Destructor. More...