Octopus
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Functions/Subroutines | |
subroutine, public | td_crank_nicolson (hm, namespace, space, gr, st, tr, time, dt, ions_dyn, ions, ext_partners, use_sparskit) |
Crank-Nicolson propagator. More... | |
subroutine | td_zop (xre, xim, yre, yim) |
operators for Crank-Nicolson scheme More... | |
subroutine | td_zopt (xre, xim, yre, yim) |
Transpose of H (called e.g. by bi-conjugate gradient solver) More... | |
subroutine | propagator_qmr_op_batch (xxb, yyb) |
operators for Crank-Nicolson scheme More... | |
subroutine | zbatch_qmr_dotu (namespace, mesh, st, xb, bb, op, max_iter, iter_used, residue, threshold, use_initial_guess) |
for complex symmetric matrices W Chen and B Poirier, J Comput Phys 219, 198-209 (2006) More... | |
Variables | |
type(namespace_t), pointer, private | namespace_p |
class(mesh_t), pointer, private | mesh_p |
type(hamiltonian_elec_t), pointer, private | hm_p |
type(propagator_base_t), pointer, private | tr_p |
type(states_elec_t), pointer, private | st_p |
integer, private | ik_op |
integer, private | ist_op |
integer, private | dim_op |
real(real64), private | t_op |
real(real64), private | dt_op |
subroutine, public propagator_cn_oct_m::td_crank_nicolson | ( | type(hamiltonian_elec_t), intent(inout), target | hm, |
type(namespace_t), intent(in), target | namespace, | ||
type(electron_space_t), intent(in) | space, | ||
type(grid_t), intent(inout), target | gr, | ||
type(states_elec_t), intent(inout), target | st, | ||
type(propagator_base_t), intent(inout), target | tr, | ||
real(real64), intent(in) | time, | ||
real(real64), intent(in) | dt, | ||
type(ion_dynamics_t), intent(inout) | ions_dyn, | ||
type(ions_t), intent(inout) | ions, | ||
type(partner_list_t), intent(in) | ext_partners, | ||
logical, intent(in) | use_sparskit | ||
) |
Crank-Nicolson propagator.
Definition at line 169 of file propagator_cn.F90.
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operators for Crank-Nicolson scheme
Definition at line 315 of file propagator_cn.F90.
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Transpose of H (called e.g. by bi-conjugate gradient solver)
Definition at line 349 of file propagator_cn.F90.
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private |
operators for Crank-Nicolson scheme
Definition at line 385 of file propagator_cn.F90.
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private |
for complex symmetric matrices W Chen and B Poirier, J Comput Phys 219, 198-209 (2006)
Adapted from linear_solver_qmr_dotp This modified version does not have the preconditioner, as it is not used for the Crank-Nicolson, which allows for improved performances
[out] | residue | the residue = abs(Ax-b) |
[in] | threshold | convergence threshold |
Definition at line 405 of file propagator_cn.F90.
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Definition at line 157 of file propagator_cn.F90.
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Definition at line 158 of file propagator_cn.F90.
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Definition at line 159 of file propagator_cn.F90.
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Definition at line 160 of file propagator_cn.F90.
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Definition at line 161 of file propagator_cn.F90.
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Definition at line 162 of file propagator_cn.F90.
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Definition at line 162 of file propagator_cn.F90.
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Definition at line 162 of file propagator_cn.F90.
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Definition at line 163 of file propagator_cn.F90.
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Definition at line 163 of file propagator_cn.F90.