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Octopus
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Data Types | |
| type | hamiltonian_elec_t |
Functions/Subroutines | |
| subroutine, public | hamiltonian_elec_init (hm, namespace, space, gr, ions, ext_partners, st, theory_level, xc, mc, kpoints, need_exchange, xc_photons) |
| subroutine, public | hamiltonian_elec_end (hm) |
| subroutine | hamiltonian_elec_release_copy_owned (hm) |
| Release owned pointer targets created by hamiltonian_elec_copy. More... | |
| subroutine, public | hamiltonian_elec_copy (hm_out, hm_in) |
| Deep-copy a hamiltonian_elec_t snapshot. More... | |
| subroutine | hamiltonian_elec_copy_guard_supported (hm_in) |
| Hard-fail guard matrix for unsupported hamiltonian snapshots. More... | |
| logical function | hamiltonian_elec_hermitian (hm) |
| pure logical function | hamiltonian_elec_needs_mgga_term (hm, terms) |
| subroutine | hamiltonian_elec_span (hm, delta, emin, namespace) |
| pure logical function, public | hamiltonian_elec_inh_term (hm) |
| subroutine, public | hamiltonian_elec_set_inh (hm, st) |
| subroutine, public | hamiltonian_elec_remove_inh (hm) |
| subroutine, public | hamiltonian_elec_adjoint (hm) |
| subroutine, public | hamiltonian_elec_not_adjoint (hm) |
| subroutine | hamiltonian_elec_update (this, mesh, namespace, space, ext_partners, time) |
| (re-)build the Hamiltonian for the next application: More... | |
| subroutine, public | hamiltonian_elec_update_pot (this, mesh, accumulate) |
| Update the KS potential of the electronic Hamiltonian. More... | |
| subroutine, public | hamiltonian_elec_epot_generate (this, namespace, space, gr, ions, ext_partners, st, time) |
| real(real64) function, public | hamiltonian_elec_get_time (this) |
| pure logical function, public | hamiltonian_elec_apply_packed (this) |
| subroutine, public | zhamiltonian_elec_apply_atom (hm, namespace, space, latt, species, pos, ia, mesh, psi, vpsi) |
| subroutine, public | hamiltonian_elec_update_with_ext_pot (this, mesh, space, ext_partners, time, mu) |
| This is an extension of "hamiltonian_elec_update_pot" to be used by the CFM4 propagator. It updates the Hamiltonian by considering a weighted sum of the external potentials at times time(1) and time(2), weighted by alpha(1) and alpha(2). More... | |
| logical function, public | hamiltonian_elec_needs_current (hm, states_are_real) |
| subroutine, public | zhamiltonian_elec_apply_all (hm, namespace, gr, st, hst) |
| logical function, public | hamiltonian_elec_has_kick (hm) |
| subroutine | hamiltonian_elec_set_mass (this, namespace, mass) |
| set the effective electron mass, checking whether it was previously redefined. More... | |
| subroutine, public | hamiltonian_elec_diagonal (hm, mesh, diag, ik) |
| subroutine | dhamiltonian_elec_apply (hm, namespace, mesh, psib, hpsib, terms, set_bc) |
| subroutine, public | dhamiltonian_elec_apply_batch (hm, namespace, mesh, psib, hpsib, terms, set_bc) |
| subroutine | dhamiltonian_elec_external (this, mesh, psib, vpsib) |
| subroutine, public | dhamiltonian_elec_apply_single (hm, namespace, mesh, psi, hpsi, ist, ik, terms, set_bc, set_phase) |
| subroutine | dh_mgga_terms (hm, mesh, psib, hpsib, lapl_psib) |
| Computes the orbital-dependent part of the mGGA potential. More... | |
| subroutine, public | dvmask (mesh, hm, st) |
| subroutine | zhamiltonian_elec_apply (hm, namespace, mesh, psib, hpsib, terms, set_bc) |
| subroutine, public | zhamiltonian_elec_apply_batch (hm, namespace, mesh, psib, hpsib, terms, set_bc) |
| subroutine, public | zhamiltonian_elec_external (this, mesh, psib, vpsib) |
| subroutine, public | zhamiltonian_elec_apply_single (hm, namespace, mesh, psi, hpsi, ist, ik, terms, set_bc, set_phase) |
| subroutine | zh_mgga_terms (hm, mesh, psib, hpsib, lapl_psib) |
| Computes the orbital-dependent part of the mGGA potential. More... | |
| subroutine, public | zvmask (mesh, hm, st) |
Variables | |
| integer, parameter, public | length = 1 |
| integer, parameter, public | velocity = 2 |
| subroutine, public hamiltonian_elec_oct_m::hamiltonian_elec_init | ( | type(hamiltonian_elec_t), intent(inout), target | hm, |
| type(namespace_t), intent(in) | namespace, | ||
| class(space_t), intent(in) | space, | ||
| type(grid_t), intent(inout), target | gr, | ||
| type(ions_t), intent(inout), target | ions, | ||
| type(partner_list_t), intent(inout) | ext_partners, | ||
| type(states_elec_t), intent(inout), target | st, | ||
| integer, intent(in) | theory_level, | ||
| type(xc_t), intent(in), target | xc, | ||
| type(multicomm_t), intent(in) | mc, | ||
| type(kpoints_t), intent(in), target | kpoints, | ||
| logical, intent(in), optional | need_exchange, | ||
| type(xc_photons_t), intent(in), optional, target | xc_photons | ||
| ) |
Definition at line 327 of file hamiltonian_elec.F90.
| subroutine, public hamiltonian_elec_oct_m::hamiltonian_elec_end | ( | type(hamiltonian_elec_t), intent(inout), target | hm | ) |
Definition at line 767 of file hamiltonian_elec.F90.
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private |
Release owned pointer targets created by hamiltonian_elec_copy.
This avoids running the full hamiltonian finalizer on shallow-alias snapshots.
Definition at line 852 of file hamiltonian_elec.F90.
| subroutine, public hamiltonian_elec_oct_m::hamiltonian_elec_copy | ( | type(hamiltonian_elec_t), intent(out), target | hm_out, |
| type(hamiltonian_elec_t), intent(inout) | hm_in | ||
| ) |
Deep-copy a hamiltonian_elec_t snapshot.
Pointer semantics:
ions is cloned and owned by the copy.der, xc, xc_photons, kpoints) are aliased.zora is cloned when present. Definition at line 901 of file hamiltonian_elec.F90.
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private |
Hard-fail guard matrix for unsupported hamiltonian snapshots.
Definition at line 1023 of file hamiltonian_elec.F90.
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private |
Definition at line 1064 of file hamiltonian_elec.F90.
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private |
Definition at line 1076 of file hamiltonian_elec.F90.
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private |
Definition at line 1097 of file hamiltonian_elec.F90.
| pure logical function, public hamiltonian_elec_oct_m::hamiltonian_elec_inh_term | ( | type(hamiltonian_elec_t), intent(in) | hm | ) |
Definition at line 1119 of file hamiltonian_elec.F90.
| subroutine, public hamiltonian_elec_oct_m::hamiltonian_elec_set_inh | ( | type(hamiltonian_elec_t), intent(inout) | hm, |
| type(states_elec_t), intent(in) | st | ||
| ) |
Definition at line 1127 of file hamiltonian_elec.F90.
| subroutine, public hamiltonian_elec_oct_m::hamiltonian_elec_remove_inh | ( | type(hamiltonian_elec_t), intent(inout) | hm | ) |
Definition at line 1142 of file hamiltonian_elec.F90.
| subroutine, public hamiltonian_elec_oct_m::hamiltonian_elec_adjoint | ( | type(hamiltonian_elec_t), intent(inout) | hm | ) |
Definition at line 1156 of file hamiltonian_elec.F90.
| subroutine, public hamiltonian_elec_oct_m::hamiltonian_elec_not_adjoint | ( | type(hamiltonian_elec_t), intent(inout) | hm | ) |
Definition at line 1173 of file hamiltonian_elec.F90.
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private |
(re-)build the Hamiltonian for the next application:
Definition at line 1191 of file hamiltonian_elec.F90.
| subroutine, public hamiltonian_elec_oct_m::hamiltonian_elec_update_pot | ( | type(hamiltonian_elec_t), intent(inout) | this, |
| class(mesh_t), intent(in) | mesh, | ||
| logical, intent(in), optional | accumulate | ||
| ) |
Update the KS potential of the electronic Hamiltonian.
Adds PCM contributions
Adds possible absorbing potential
Definition at line 1418 of file hamiltonian_elec.F90.
| subroutine, public hamiltonian_elec_oct_m::hamiltonian_elec_epot_generate | ( | type(hamiltonian_elec_t), intent(inout) | this, |
| type(namespace_t), intent(in) | namespace, | ||
| class(electron_space_t), intent(in) | space, | ||
| type(grid_t), intent(in) | gr, | ||
| type(ions_t), intent(inout), target | ions, | ||
| type(partner_list_t), intent(in) | ext_partners, | ||
| type(states_elec_t), intent(inout) | st, | ||
| real(real64), intent(in), optional | time | ||
| ) |
Generates the real-space PCM potential due to nuclei which do not change during the SCF calculation.
Local field effects due to static electrostatic potentials (if they were). The laser and the kick are included in subroutine v_ks_hartree (module v_ks).
Definition at line 1521 of file hamiltonian_elec.F90.
| real(real64) function, public hamiltonian_elec_oct_m::hamiltonian_elec_get_time | ( | type(hamiltonian_elec_t), intent(inout) | this | ) |
Definition at line 1604 of file hamiltonian_elec.F90.
| pure logical function, public hamiltonian_elec_oct_m::hamiltonian_elec_apply_packed | ( | class(hamiltonian_elec_t), intent(in) | this | ) |
Definition at line 1612 of file hamiltonian_elec.F90.
| subroutine, public hamiltonian_elec_oct_m::zhamiltonian_elec_apply_atom | ( | type(hamiltonian_elec_t), intent(in) | hm, |
| type(namespace_t), intent(in) | namespace, | ||
| class(space_t), intent(in) | space, | ||
| type(lattice_vectors_t), intent(in) | latt, | ||
| class(species_t), intent(in) | species, | ||
| real(real64), dimension(1:space%dim), intent(in) | pos, | ||
| integer, intent(in) | ia, | ||
| class(mesh_t), intent(in) | mesh, | ||
| complex(real64), dimension(:,:), intent(in) | psi, | ||
| complex(real64), dimension(:,:), intent(out) | vpsi | ||
| ) |
| [in] | psi | (grnp_part, hmddim) |
| [out] | vpsi | (grnp, hmddim) |
Definition at line 1621 of file hamiltonian_elec.F90.
| subroutine, public hamiltonian_elec_oct_m::hamiltonian_elec_update_with_ext_pot | ( | type(hamiltonian_elec_t), intent(inout) | this, |
| class(mesh_t), intent(in) | mesh, | ||
| class(space_t), intent(in) | space, | ||
| type(partner_list_t), intent(in) | ext_partners, | ||
| real(real64), dimension(1:2), intent(in) | time, | ||
| real(real64), dimension(1:2), intent(in) | mu | ||
| ) |
This is an extension of "hamiltonian_elec_update_pot" to be used by the CFM4 propagator. It updates the Hamiltonian by considering a weighted sum of the external potentials at times time(1) and time(2), weighted by alpha(1) and alpha(2).
Definition at line 1654 of file hamiltonian_elec.F90.
| logical function, public hamiltonian_elec_oct_m::hamiltonian_elec_needs_current | ( | type(hamiltonian_elec_t), intent(in) | hm, |
| logical, intent(in) | states_are_real | ||
| ) |
Definition at line 1848 of file hamiltonian_elec.F90.
| subroutine, public hamiltonian_elec_oct_m::zhamiltonian_elec_apply_all | ( | type(hamiltonian_elec_t), intent(inout) | hm, |
| type(namespace_t), intent(in) | namespace, | ||
| type(grid_t), intent(in) | gr, | ||
| type(states_elec_t), intent(inout) | st, | ||
| type(states_elec_t), intent(inout) | hst | ||
| ) |
Definition at line 1866 of file hamiltonian_elec.F90.
| logical function, public hamiltonian_elec_oct_m::hamiltonian_elec_has_kick | ( | type(hamiltonian_elec_t), intent(in) | hm | ) |
Definition at line 1913 of file hamiltonian_elec.F90.
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private |
set the effective electron mass, checking whether it was previously redefined.
Definition at line 1925 of file hamiltonian_elec.F90.
| subroutine, public hamiltonian_elec_oct_m::hamiltonian_elec_diagonal | ( | type(hamiltonian_elec_t), intent(in) | hm, |
| class(mesh_t), intent(in) | mesh, | ||
| real(real64), dimension(:,:), intent(out), contiguous | diag, | ||
| integer, intent(in) | ik | ||
| ) |
| [out] | diag | hpsi(grmeshnp, hmdnspin) |
Definition at line 1943 of file hamiltonian_elec.F90.
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| [in] | set_bc | If set to .false. the boundary conditions are assumed to be set previously. |
Definition at line 2054 of file hamiltonian_elec.F90.
| subroutine, public hamiltonian_elec_oct_m::dhamiltonian_elec_apply_batch | ( | type(hamiltonian_elec_t), intent(in) | hm, |
| type(namespace_t), intent(in) | namespace, | ||
| class(mesh_t), intent(in) | mesh, | ||
| type(wfs_elec_t), intent(inout), target | psib, | ||
| type(wfs_elec_t), intent(inout), target | hpsib, | ||
| integer, intent(in), optional | terms, | ||
| logical, intent(in), optional | set_bc | ||
| ) |
| [in] | set_bc | If set to .false. the boundary conditions are assumed to be set previously. |
Definition at line 2083 of file hamiltonian_elec.F90.
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private |
Definition at line 2299 of file hamiltonian_elec.F90.
| subroutine, public hamiltonian_elec_oct_m::dhamiltonian_elec_apply_single | ( | type(hamiltonian_elec_t), intent(in) | hm, |
| type(namespace_t), intent(in) | namespace, | ||
| class(mesh_t), intent(in) | mesh, | ||
| real(real64), dimension(:,:), intent(inout), target, contiguous | psi, | ||
| real(real64), dimension(:,:), intent(inout), target, contiguous | hpsi, | ||
| integer, intent(in) | ist, | ||
| integer, intent(in) | ik, | ||
| integer, intent(in), optional | terms, | ||
| logical, intent(in), optional | set_bc, | ||
| logical, intent(in), optional | set_phase | ||
| ) |
| [in] | ist | the index of the state |
| [in] | ik | the index of the k-point |
| [in,out] | psi | (grmeshnp_part, hmddim) |
| [in,out] | hpsi | (grmeshnp, hmddim) |
Definition at line 2348 of file hamiltonian_elec.F90.
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private |
Computes the orbital-dependent part of the mGGA potential.
This reads as \( L\psi =-\nabla \cdot [\vtau \nabla \psi]\).
It is trivial to show that this operator is self-adjoint. However, this is never the case with finite differences. This is thus reimplemented as L\psi = -1/2(v_\tau \Delta \psi - \psi \Delta[v_\tau] + \Delta [v_\tau \psi]
The same expression was proposed in Richter et al., J. Chem. Phys. 159, 124117 (2023).
Definition at line 2392 of file hamiltonian_elec.F90.
| subroutine, public hamiltonian_elec_oct_m::dvmask | ( | class(mesh_t), intent(in) | mesh, |
| type(hamiltonian_elec_t), intent(in) | hm, | ||
| type(states_elec_t), intent(inout) | st | ||
| ) |
Definition at line 2442 of file hamiltonian_elec.F90.
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private |
| [in] | set_bc | If set to .false. the boundary conditions are assumed to be set previously. |
Definition at line 2546 of file hamiltonian_elec.F90.
| subroutine, public hamiltonian_elec_oct_m::zhamiltonian_elec_apply_batch | ( | type(hamiltonian_elec_t), intent(in) | hm, |
| type(namespace_t), intent(in) | namespace, | ||
| class(mesh_t), intent(in) | mesh, | ||
| type(wfs_elec_t), intent(inout), target | psib, | ||
| type(wfs_elec_t), intent(inout), target | hpsib, | ||
| integer, intent(in), optional | terms, | ||
| logical, intent(in), optional | set_bc | ||
| ) |
| [in] | set_bc | If set to .false. the boundary conditions are assumed to be set previously. |
Definition at line 2575 of file hamiltonian_elec.F90.
| subroutine, public hamiltonian_elec_oct_m::zhamiltonian_elec_external | ( | type(hamiltonian_elec_t), intent(in) | this, |
| class(mesh_t), intent(in) | mesh, | ||
| type(wfs_elec_t), intent(in) | psib, | ||
| type(wfs_elec_t), intent(inout) | vpsib | ||
| ) |
Definition at line 2791 of file hamiltonian_elec.F90.
| subroutine, public hamiltonian_elec_oct_m::zhamiltonian_elec_apply_single | ( | type(hamiltonian_elec_t), intent(in) | hm, |
| type(namespace_t), intent(in) | namespace, | ||
| class(mesh_t), intent(in) | mesh, | ||
| complex(real64), dimension(:,:), intent(inout), target, contiguous | psi, | ||
| complex(real64), dimension(:,:), intent(inout), target, contiguous | hpsi, | ||
| integer, intent(in) | ist, | ||
| integer, intent(in) | ik, | ||
| integer, intent(in), optional | terms, | ||
| logical, intent(in), optional | set_bc, | ||
| logical, intent(in), optional | set_phase | ||
| ) |
| [in] | ist | the index of the state |
| [in] | ik | the index of the k-point |
| [in,out] | psi | (grmeshnp_part, hmddim) |
| [in,out] | hpsi | (grmeshnp, hmddim) |
Definition at line 2840 of file hamiltonian_elec.F90.
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private |
Computes the orbital-dependent part of the mGGA potential.
This reads as \( L\psi =-\nabla \cdot [\vtau \nabla \psi]\).
It is trivial to show that this operator is self-adjoint. However, this is never the case with finite differences. This is thus reimplemented as L\psi = -1/2(v_\tau \Delta \psi - \psi \Delta[v_\tau] + \Delta [v_\tau \psi]
The same expression was proposed in Richter et al., J. Chem. Phys. 159, 124117 (2023).
Definition at line 2884 of file hamiltonian_elec.F90.
| subroutine, public hamiltonian_elec_oct_m::zvmask | ( | class(mesh_t), intent(in) | mesh, |
| type(hamiltonian_elec_t), intent(in) | hm, | ||
| type(states_elec_t), intent(inout) | st | ||
| ) |
Definition at line 2934 of file hamiltonian_elec.F90.
| integer, parameter, public hamiltonian_elec_oct_m::length = 1 |
Definition at line 319 of file hamiltonian_elec.F90.
| integer, parameter, public hamiltonian_elec_oct_m::velocity = 2 |
Definition at line 319 of file hamiltonian_elec.F90.