Octopus
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Data Types | |
type | current_t |
Functions/Subroutines | |
subroutine, public | current_init (this, namespace) |
subroutine | current_batch_accumulate (st, der, ik, ib, psib, gpsib) |
subroutine, public | current_calculate (this, namespace, gr, hm, space, st) |
Compute total electronic current density. More... | |
subroutine | current_calculate_dia_non_unif_vec_pot (der, hm, st) |
Compute diamagnetic current density from non-uniform vector potential (the part coming from the uniform vector potential is already included in the paramagnetic term) More... | |
subroutine, public | current_calculate_mag (der, st) |
Compute magnetization current Note: due to the the numerical curl, the magnetization current could deviate from the analytical one near the origin (see test for "current_density"). More... | |
subroutine | current_calculate_para (this, namespace, gr, hm, space, st) |
Compute paramagnetic current density (including full diamagnetic term if method = Hamiltonian us used, and including diamagnetic from uniform vector potential otherwise) More... | |
subroutine, public | current_calculate_mel (der, hm, psi_i, psi_j, ik, cmel) |
subroutine, public | current_heat_calculate (space, der, hm, st, current) |
Variables | |
integer, parameter, public | current_gradient = 1 |
integer, parameter, public | current_gradient_corr = 2 |
integer, parameter, public | current_hamiltonian = 3 |
subroutine, public current_oct_m::current_init | ( | type(current_t), intent(out) | this, |
type(namespace_t), intent(in) | namespace | ||
) |
Definition at line 176 of file current.F90.
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private |
Definition at line 224 of file current.F90.
subroutine, public current_oct_m::current_calculate | ( | type(current_t), intent(in) | this, |
type(namespace_t), intent(in) | namespace, | ||
type(grid_t), intent(inout) | gr, | ||
type(hamiltonian_elec_t), intent(in) | hm, | ||
class(space_t), intent(in) | space, | ||
type(states_elec_t), intent(inout) | st | ||
) |
Compute total electronic current density.
Definition at line 366 of file current.F90.
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private |
Compute diamagnetic current density from non-uniform vector potential (the part coming from the uniform vector potential is already included in the paramagnetic term)
Definition at line 394 of file current.F90.
subroutine, public current_oct_m::current_calculate_mag | ( | type(derivatives_t), intent(inout) | der, |
type(states_elec_t), intent(inout) | st | ||
) |
Compute magnetization current Note: due to the the numerical curl, the magnetization current could deviate from the analytical one near the origin (see test for "current_density").
Definition at line 429 of file current.F90.
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private |
Compute paramagnetic current density (including full diamagnetic term if method = Hamiltonian us used, and including diamagnetic from uniform vector potential otherwise)
Definition at line 468 of file current.F90.
subroutine, public current_oct_m::current_calculate_mel | ( | type(derivatives_t), intent(inout) | der, |
type(hamiltonian_elec_t), intent(in) | hm, | ||
complex(real64), dimension(:,:), intent(in) | psi_i, | ||
complex(real64), dimension(:,:), intent(in) | psi_j, | ||
integer, intent(in) | ik, | ||
complex(real64), dimension(:,:), intent(out) | cmel | ||
) |
Definition at line 763 of file current.F90.
subroutine, public current_oct_m::current_heat_calculate | ( | class(space_t), intent(in) | space, |
type(derivatives_t), intent(in) | der, | ||
type(hamiltonian_elec_t), intent(in) | hm, | ||
type(states_elec_t), intent(in) | st, | ||
real(real64), dimension(:, :, :), intent(out) | current | ||
) |
Definition at line 858 of file current.F90.
integer, parameter, public current_oct_m::current_gradient = 1 |
Definition at line 169 of file current.F90.
integer, parameter, public current_oct_m::current_gradient_corr = 2 |
Definition at line 169 of file current.F90.
integer, parameter, public current_oct_m::current_hamiltonian = 3 |
Definition at line 169 of file current.F90.