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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 217 of file xc_oep.F90.
| subroutine, public xc_oep_oct_m::xc_oep_end | ( | class(xc_oep_t), intent(inout) | oep | ) |
Definition at line 356 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 378 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 396 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 418 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 471 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 553 of file xc_oep.F90.
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private |
Definition at line 869 of file xc_oep.F90.
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private |
Definition at line 906 of file xc_oep.F90.
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private |
Definition at line 924 of file xc_oep.F90.
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private |
This routine calculates the SIC functional for the spinor case.
Definition at line 961 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 1139 of file xc_oep.F90.
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private |
This routine calculates the SIC exchange functional.
Definition at line 1410 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 1535 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 1729 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 2015 of file xc_oep.F90.
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private |
This routine calculates the SIC exchange functional.
Definition at line 2286 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 2411 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 2605 of file xc_oep.F90.
| integer, parameter, public xc_oep_oct_m::oep_level_none = 1 |
the OEP levels
Definition at line 173 of file xc_oep.F90.
| integer, parameter, public xc_oep_oct_m::oep_level_kli = 3 |
Definition at line 173 of file xc_oep.F90.
| integer, parameter, public xc_oep_oct_m::oep_level_full = 5 |
Definition at line 173 of file xc_oep.F90.
| integer, parameter, public xc_oep_oct_m::oep_mixing_scheme_const = 1 |
Mixing schemes.
Definition at line 179 of file xc_oep.F90.
| integer, parameter, public xc_oep_oct_m::oep_mixing_scheme_bb = 2 |
Definition at line 179 of file xc_oep.F90.
| integer, parameter, public xc_oep_oct_m::oep_mixing_scheme_dens = 3 |
Definition at line 179 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 185 of file xc_oep.F90.
| integer, parameter, public xc_oep_oct_m::oep_type_mgga = 2 |
Definition at line 185 of file xc_oep.F90.
| integer, parameter, public xc_oep_oct_m::oep_type_sic = 3 |
Definition at line 185 of file xc_oep.F90.
| integer, parameter, public xc_oep_oct_m::oep_type_photons = 4 |
Definition at line 185 of file xc_oep.F90.