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Octopus
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Data Types | |
| type | xc_oep_t |
Functions/Subroutines | |
| subroutine, public | xc_oep_init (oep, namespace, gr, st, mc, space, oep_type) |
| subroutine, public | xc_oep_end (oep) |
| subroutine, public | xc_oep_write_info (oep, iunit, namespace) |
| subroutine, public | xc_oep_spinfactor (oep, nspin) |
| A couple of auxiliary functions for oep. More... | |
| subroutine, public | xc_oep_analyzeeigen (oep, st, is) |
| subroutine, public | xc_oep_mix (oep, mesh, ss, rho, is) |
| A routine that takes care of mixing the potential. More... | |
| subroutine | xc_kli_pauli_solve (mesh, st, oep) |
| Explicit solution of the KLI equation for Pauli spinors. More... | |
| subroutine | get_rotation_matrix (dens, alpha, betar, betai) |
| subroutine | rotate_to_local (mat, alpha, betar, betai, alpha2, beta2, rot_mat) |
| subroutine | rotate_to_global (mat, alpha, betar, betai, alpha2, beta2, rot_mat) |
| subroutine | oep_sic_pauli (xcs, gr, psolver, namespace, space, rcell_volume, st, kpoints, oep, ex, ec) |
| This routine calculates the SIC functional for the spinor case. More... | |
| subroutine | dxc_kli_solve (space, mesh, st, oep, rcell_volume) |
| This routine solves the KLI approximation to the OEP equation. More... | |
| subroutine | doep_sic (xcs, gr, psolver, namespace, space, rcell_volume, st, kpoints, is, oep, ex, ec) |
| This routine calculates the SIC exchange functional. More... | |
| subroutine, public | dxc_oep_calc (oep, namespace, xcs, gr, hm, st, space, rcell_volume, ex, ec, vxc) |
| This file handles the evaluation of the OEP potential, in the KLI or full OEP as described in S. Kuemmel and J. Perdew, PRL 90, 043004 (2003) More... | |
| subroutine | dxc_oep_solve (namespace, space, mesh, hm, st, is, rcell_volume, vxc, oep) |
| This routine follows closely the one of PRB 68, 035103 (2003) Below we refer to the equation number of this paper. More... | |
| subroutine | zxc_kli_solve (space, mesh, st, oep, rcell_volume) |
| This routine solves the KLI approximation to the OEP equation. More... | |
| subroutine | zoep_sic (xcs, gr, psolver, namespace, space, rcell_volume, st, kpoints, is, oep, ex, ec) |
| This routine calculates the SIC exchange functional. More... | |
| subroutine, public | zxc_oep_calc (oep, namespace, xcs, gr, hm, st, space, rcell_volume, ex, ec, vxc) |
| This file handles the evaluation of the OEP potential, in the KLI or full OEP as described in S. Kuemmel and J. Perdew, PRL 90, 043004 (2003) More... | |
| subroutine | zxc_oep_solve (namespace, space, mesh, hm, st, is, rcell_volume, vxc, oep) |
| This routine follows closely the one of PRB 68, 035103 (2003) Below we refer to the equation number of this paper. More... | |
Variables | |
| integer, parameter, public | oep_level_none = 1 |
| the OEP levels More... | |
| integer, parameter, public | oep_level_kli = 3 |
| integer, parameter, public | oep_level_full = 5 |
| integer, parameter, public | oep_mixing_scheme_const = 1 |
| Mixing schemes. More... | |
| integer, parameter, public | oep_mixing_scheme_bb = 2 |
| integer, parameter, public | oep_mixing_scheme_dens = 3 |
| integer, parameter, public | oep_type_exx = 1 |
| The different types of OEP that we can work with. More... | |
| integer, parameter, public | oep_type_mgga = 2 |
| integer, parameter, public | oep_type_sic = 3 |
| integer, parameter, public | oep_type_photons = 4 |
| subroutine, public xc_oep_oct_m::xc_oep_init | ( | type(xc_oep_t), intent(inout) | oep, |
| type(namespace_t), intent(in) | namespace, | ||
| type(grid_t), intent(inout) | gr, | ||
| type(states_elec_t), intent(in) | st, | ||
| type(multicomm_t), intent(in) | mc, | ||
| class(space_t), intent(in) | space, | ||
| integer, intent(in) | oep_type | ||
| ) |
Definition at line 215 of file xc_oep.F90.
| subroutine, public xc_oep_oct_m::xc_oep_end | ( | class(xc_oep_t), intent(inout) | oep | ) |
Definition at line 354 of file xc_oep.F90.
| subroutine, public xc_oep_oct_m::xc_oep_write_info | ( | type(xc_oep_t), intent(in) | oep, |
| integer, intent(in), optional | iunit, | ||
| type(namespace_t), intent(in), optional | namespace | ||
| ) |
Definition at line 376 of file xc_oep.F90.
| subroutine, public xc_oep_oct_m::xc_oep_spinfactor | ( | class(xc_oep_t), intent(inout) | oep, |
| integer, intent(in) | nspin | ||
| ) |
A couple of auxiliary functions for oep.
Definition at line 394 of file xc_oep.F90.
| subroutine, public xc_oep_oct_m::xc_oep_analyzeeigen | ( | class(xc_oep_t), intent(inout) | oep, |
| type(states_elec_t), intent(in) | st, | ||
| integer, intent(in) | is | ||
| ) |
| [in] | is | spin/k-point index |
Definition at line 416 of file xc_oep.F90.
| subroutine, public xc_oep_oct_m::xc_oep_mix | ( | class(xc_oep_t), intent(inout) | oep, |
| type(mesh_t), intent(in) | mesh, | ||
| real(real64), dimension(:), intent(in), contiguous | ss, | ||
| real(real64), dimension(:), intent(in), contiguous | rho, | ||
| integer, intent(in) | is | ||
| ) |
A routine that takes care of mixing the potential.
Definition at line 469 of file xc_oep.F90.
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private |
Explicit solution of the KLI equation for Pauli spinors.
More precisely, this implements the explicit solution of Eq. F12 of Tancogne-Dejean et al., PRB 107, 165111 (2023).
Definition at line 551 of file xc_oep.F90.
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private |
Definition at line 867 of file xc_oep.F90.
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private |
Definition at line 904 of file xc_oep.F90.
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private |
Definition at line 922 of file xc_oep.F90.
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private |
This routine calculates the SIC functional for the spinor case.
Definition at line 959 of file xc_oep.F90.
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private |
This routine solves the KLI approximation to the OEP equation.
This implements the direct solution of the KLI equation.
Definition at line 1137 of file xc_oep.F90.
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private |
This routine calculates the SIC exchange functional.
Definition at line 1408 of file xc_oep.F90.
| subroutine, public xc_oep_oct_m::dxc_oep_calc | ( | type(xc_oep_t), intent(inout) | oep, |
| type(namespace_t), intent(in) | namespace, | ||
| type(xc_t), intent(inout) | xcs, | ||
| type(grid_t), intent(in) | gr, | ||
| type(hamiltonian_elec_t), intent(inout) | hm, | ||
| type(states_elec_t), intent(inout), target | st, | ||
| class(space_t), intent(in) | space, | ||
| real(real64), intent(in) | rcell_volume, | ||
| real(real64), intent(inout) | ex, | ||
| real(real64), intent(inout) | ec, | ||
| real(real64), dimension(:,:), intent(inout), optional, contiguous | vxc | ||
| ) |
This file handles the evaluation of the OEP potential, in the KLI or full OEP as described in S. Kuemmel and J. Perdew, PRL 90, 043004 (2003)
This file has to be outside the module xc, for it requires the Hpsi. This is why it needs the xc_functional module. I prefer to put it here since the rest of the Hamiltonian module does not know about the gory details of how xc is defined and calculated.
| [in,out] | vxc | vxc(meshnp, stdnspin) |
Definition at line 1533 of file xc_oep.F90.
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private |
This routine follows closely the one of PRB 68, 035103 (2003) Below we refer to the equation number of this paper.
| [in,out] | vxc | (meshnp, given for the spin is) |
Definition at line 1727 of file xc_oep.F90.
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private |
This routine solves the KLI approximation to the OEP equation.
This implements the direct solution of the KLI equation.
Definition at line 2013 of file xc_oep.F90.
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private |
This routine calculates the SIC exchange functional.
Definition at line 2284 of file xc_oep.F90.
| subroutine, public xc_oep_oct_m::zxc_oep_calc | ( | type(xc_oep_t), intent(inout) | oep, |
| type(namespace_t), intent(in) | namespace, | ||
| type(xc_t), intent(inout) | xcs, | ||
| type(grid_t), intent(in) | gr, | ||
| type(hamiltonian_elec_t), intent(inout) | hm, | ||
| type(states_elec_t), intent(inout), target | st, | ||
| class(space_t), intent(in) | space, | ||
| real(real64), intent(in) | rcell_volume, | ||
| real(real64), intent(inout) | ex, | ||
| real(real64), intent(inout) | ec, | ||
| real(real64), dimension(:,:), intent(inout), optional, contiguous | vxc | ||
| ) |
This file handles the evaluation of the OEP potential, in the KLI or full OEP as described in S. Kuemmel and J. Perdew, PRL 90, 043004 (2003)
This file has to be outside the module xc, for it requires the Hpsi. This is why it needs the xc_functional module. I prefer to put it here since the rest of the Hamiltonian module does not know about the gory details of how xc is defined and calculated.
| [in,out] | vxc | vxc(meshnp, stdnspin) |
Definition at line 2409 of file xc_oep.F90.
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private |
This routine follows closely the one of PRB 68, 035103 (2003) Below we refer to the equation number of this paper.
| [in,out] | vxc | (meshnp, given for the spin is) |
Definition at line 2603 of file xc_oep.F90.
| integer, parameter, public xc_oep_oct_m::oep_level_none = 1 |
the OEP levels
Definition at line 171 of file xc_oep.F90.
| integer, parameter, public xc_oep_oct_m::oep_level_kli = 3 |
Definition at line 171 of file xc_oep.F90.
| integer, parameter, public xc_oep_oct_m::oep_level_full = 5 |
Definition at line 171 of file xc_oep.F90.
| integer, parameter, public xc_oep_oct_m::oep_mixing_scheme_const = 1 |
Mixing schemes.
Definition at line 177 of file xc_oep.F90.
| integer, parameter, public xc_oep_oct_m::oep_mixing_scheme_bb = 2 |
Definition at line 177 of file xc_oep.F90.
| integer, parameter, public xc_oep_oct_m::oep_mixing_scheme_dens = 3 |
Definition at line 177 of file xc_oep.F90.
| integer, parameter, public xc_oep_oct_m::oep_type_exx = 1 |
The different types of OEP that we can work with.
Definition at line 183 of file xc_oep.F90.
| integer, parameter, public xc_oep_oct_m::oep_type_mgga = 2 |
Definition at line 183 of file xc_oep.F90.
| integer, parameter, public xc_oep_oct_m::oep_type_sic = 3 |
Definition at line 183 of file xc_oep.F90.
| integer, parameter, public xc_oep_oct_m::oep_type_photons = 4 |
Definition at line 183 of file xc_oep.F90.