Merge branch 'master' of https://github.com/eginer/quantum_package into eginer-master
Conflicts: plugins/CISD/README.rst plugins/CISD_SC2_selected/README.rst plugins/CISD_selected/README.rst plugins/DDCI_selected/README.rst plugins/MRCC_CASSD/.gitignore src/Determinants/davidson.irp.f src/Determinants/slater_rules.irp.f src/Ezfio_files/README.rst
6
ocaml/.gitignore
vendored
@ -38,12 +38,12 @@ qp_print
|
||||
qp_run
|
||||
qp_set_ddci
|
||||
qp_set_mo_class
|
||||
Input_determinants.ml
|
||||
Input_hartree_fock.ml
|
||||
Input_integrals_bielec.ml
|
||||
Input_pseudo.ml
|
||||
Input_perturbation.ml
|
||||
Input_properties.ml
|
||||
Input_pseudo.ml
|
||||
Input_determinants.ml
|
||||
Input_hartree_fock.ml
|
||||
qp_edit.ml
|
||||
qp_edit
|
||||
qp_edit.native
|
||||
|
1
plugins/CAS_SD/.gitignore
vendored
@ -24,6 +24,7 @@ Selectors_full
|
||||
Utils
|
||||
cas_sd
|
||||
cas_sd_selected
|
||||
cas_sd_selected_no_skip
|
||||
ezfio_interface.irp.f
|
||||
irpf90.make
|
||||
irpf90_entities
|
||||
|
@ -13,11 +13,11 @@ Documentation
|
||||
.. Do not edit this section. It was auto-generated from the
|
||||
.. by the `update_README.py` script.
|
||||
|
||||
`full_ci <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/cas_sd_selected.irp.f#L1>`_
|
||||
`full_ci <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/cas_sd_selected_no_skip.irp.f#L1>`_
|
||||
Undocumented
|
||||
|
||||
|
||||
`h_apply_cas_sd <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L408>`_
|
||||
`h_apply_cas_sd <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L414>`_
|
||||
Calls H_apply on the HF determinant and selects all connected single and double
|
||||
excitations (of the same symmetry). Auto-generated by the ``generate_h_apply`` script.
|
||||
|
||||
@ -28,58 +28,58 @@ Documentation
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_cas_sd_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L264>`_
|
||||
`h_apply_cas_sd_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L269>`_
|
||||
Generate all single excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_cas_sd_pt2 <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L2586>`_
|
||||
`h_apply_cas_sd_pt2 <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L2610>`_
|
||||
Calls H_apply on the HF determinant and selects all connected single and double
|
||||
excitations (of the same symmetry). Auto-generated by the ``generate_h_apply`` script.
|
||||
|
||||
|
||||
`h_apply_cas_sd_pt2_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L2100>`_
|
||||
`h_apply_cas_sd_pt2_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L2118>`_
|
||||
Generate all double excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_cas_sd_pt2_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L2404>`_
|
||||
`h_apply_cas_sd_pt2_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L2427>`_
|
||||
Generate all single excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_cas_sd_selected <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L1854>`_
|
||||
`h_apply_cas_sd_selected <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L1872>`_
|
||||
Calls H_apply on the HF determinant and selects all connected single and double
|
||||
excitations (of the same symmetry). Auto-generated by the ``generate_h_apply`` script.
|
||||
|
||||
|
||||
`h_apply_cas_sd_selected_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L1334>`_
|
||||
`h_apply_cas_sd_selected_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L1346>`_
|
||||
Generate all double excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_cas_sd_selected_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L1658>`_
|
||||
`h_apply_cas_sd_selected_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L1675>`_
|
||||
Generate all single excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_cas_sd_selected_no_skip <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L1116>`_
|
||||
`h_apply_cas_sd_selected_no_skip <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L1128>`_
|
||||
Calls H_apply on the HF determinant and selects all connected single and double
|
||||
excitations (of the same symmetry). Auto-generated by the ``generate_h_apply`` script.
|
||||
|
||||
|
||||
`h_apply_cas_sd_selected_no_skip_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L596>`_
|
||||
`h_apply_cas_sd_selected_no_skip_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L602>`_
|
||||
Generate all double excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_cas_sd_selected_no_skip_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L920>`_
|
||||
`h_apply_cas_sd_selected_no_skip_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/CAS_SD/H_apply.irp.f_shell_22#L931>`_
|
||||
Generate all single excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
Before Width: | Height: | Size: 100 KiB After Width: | Height: | Size: 111 KiB |
@ -43,7 +43,6 @@ Documentation
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_cisd_selection_dipole_moment_z_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/CISD_selected/H_apply.irp.f_shell_10#L4921>`_
|
||||
Generate all single excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
|
@ -14,7 +14,7 @@ Documentation
|
||||
Undocumented
|
||||
|
||||
|
||||
`h_apply_fci <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L521>`_
|
||||
`h_apply_fci <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L527>`_
|
||||
Calls H_apply on the HF determinant and selects all connected single and double
|
||||
excitations (of the same symmetry). Auto-generated by the ``generate_h_apply`` script.
|
||||
|
||||
@ -25,126 +25,126 @@ Documentation
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_fci_mono <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L2720>`_
|
||||
`h_apply_fci_mono <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L2744>`_
|
||||
Calls H_apply on the HF determinant and selects all connected single and double
|
||||
excitations (of the same symmetry). Auto-generated by the ``generate_h_apply`` script.
|
||||
|
||||
|
||||
`h_apply_fci_mono_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L2198>`_
|
||||
`h_apply_fci_mono_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L2216>`_
|
||||
Generate all double excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_fci_mono_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L2522>`_
|
||||
`h_apply_fci_mono_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L2545>`_
|
||||
Generate all single excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_fci_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L325>`_
|
||||
`h_apply_fci_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L330>`_
|
||||
Generate all single excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_fci_no_skip <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L1980>`_
|
||||
`h_apply_fci_no_skip <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L1998>`_
|
||||
Calls H_apply on the HF determinant and selects all connected single and double
|
||||
excitations (of the same symmetry). Auto-generated by the ``generate_h_apply`` script.
|
||||
|
||||
|
||||
`h_apply_fci_no_skip_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L1460>`_
|
||||
`h_apply_fci_no_skip_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L1472>`_
|
||||
Generate all double excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_fci_no_skip_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L1784>`_
|
||||
`h_apply_fci_no_skip_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L1801>`_
|
||||
Generate all single excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_fci_pt2 <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L1253>`_
|
||||
`h_apply_fci_pt2 <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L1265>`_
|
||||
Calls H_apply on the HF determinant and selects all connected single and double
|
||||
excitations (of the same symmetry). Auto-generated by the ``generate_h_apply`` script.
|
||||
|
||||
|
||||
`h_apply_fci_pt2_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L767>`_
|
||||
`h_apply_fci_pt2_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L773>`_
|
||||
Generate all double excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_fci_pt2_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L1071>`_
|
||||
`h_apply_fci_pt2_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L1082>`_
|
||||
Generate all single excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_pt2_mono_delta_rho <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L4222>`_
|
||||
`h_apply_pt2_mono_delta_rho <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L4258>`_
|
||||
Calls H_apply on the HF determinant and selects all connected single and double
|
||||
excitations (of the same symmetry). Auto-generated by the ``generate_h_apply`` script.
|
||||
|
||||
|
||||
`h_apply_pt2_mono_delta_rho_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L3734>`_
|
||||
`h_apply_pt2_mono_delta_rho_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L3764>`_
|
||||
Generate all double excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_pt2_mono_delta_rho_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L4038>`_
|
||||
`h_apply_pt2_mono_delta_rho_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L4073>`_
|
||||
Generate all single excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_pt2_mono_di_delta_rho <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L5681>`_
|
||||
`h_apply_pt2_mono_di_delta_rho <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L5729>`_
|
||||
Calls H_apply on the HF determinant and selects all connected single and double
|
||||
excitations (of the same symmetry). Auto-generated by the ``generate_h_apply`` script.
|
||||
|
||||
|
||||
`h_apply_pt2_mono_di_delta_rho_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L5195>`_
|
||||
`h_apply_pt2_mono_di_delta_rho_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L5237>`_
|
||||
Generate all double excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_pt2_mono_di_delta_rho_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L5499>`_
|
||||
`h_apply_pt2_mono_di_delta_rho_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L5546>`_
|
||||
Generate all single excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_select_mono_delta_rho <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L3488>`_
|
||||
`h_apply_select_mono_delta_rho <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L3518>`_
|
||||
Calls H_apply on the HF determinant and selects all connected single and double
|
||||
excitations (of the same symmetry). Auto-generated by the ``generate_h_apply`` script.
|
||||
|
||||
|
||||
`h_apply_select_mono_delta_rho_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L2966>`_
|
||||
`h_apply_select_mono_delta_rho_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L2990>`_
|
||||
Generate all double excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_select_mono_delta_rho_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L3290>`_
|
||||
`h_apply_select_mono_delta_rho_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L3319>`_
|
||||
Generate all single excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_select_mono_di_delta_rho <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L4949>`_
|
||||
`h_apply_select_mono_di_delta_rho <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L4991>`_
|
||||
Calls H_apply on the HF determinant and selects all connected single and double
|
||||
excitations (of the same symmetry). Auto-generated by the ``generate_h_apply`` script.
|
||||
|
||||
|
||||
`h_apply_select_mono_di_delta_rho_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L4429>`_
|
||||
`h_apply_select_mono_di_delta_rho_diexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L4465>`_
|
||||
Generate all double excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_select_mono_di_delta_rho_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L4753>`_
|
||||
`h_apply_select_mono_di_delta_rho_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/Full_CI/H_apply.irp.f_shell_43#L4794>`_
|
||||
Generate all single excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
Before Width: | Height: | Size: 98 KiB After Width: | Height: | Size: 111 KiB |
Before Width: | Height: | Size: 61 KiB After Width: | Height: | Size: 69 KiB |
Before Width: | Height: | Size: 73 KiB After Width: | Height: | Size: 82 KiB |
Before Width: | Height: | Size: 57 KiB After Width: | Height: | Size: 66 KiB |
@ -94,7 +94,7 @@ Documentation
|
||||
Undocumented
|
||||
|
||||
|
||||
`h_apply_mrcc <http://github.com/LCPQ/quantum_package/tree/master/src/MRCC_Utils/H_apply.irp.f_shell_27#L416>`_
|
||||
`h_apply_mrcc <http://github.com/LCPQ/quantum_package/tree/master/src/MRCC_Utils/H_apply.irp.f_shell_27#L422>`_
|
||||
Calls H_apply on the HF determinant and selects all connected single and double
|
||||
excitations (of the same symmetry). Auto-generated by the ``generate_h_apply`` script.
|
||||
|
||||
@ -105,7 +105,7 @@ Documentation
|
||||
Assume N_int is already provided.
|
||||
|
||||
|
||||
`h_apply_mrcc_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/MRCC_Utils/H_apply.irp.f_shell_27#L268>`_
|
||||
`h_apply_mrcc_monoexc <http://github.com/LCPQ/quantum_package/tree/master/src/MRCC_Utils/H_apply.irp.f_shell_27#L273>`_
|
||||
Generate all single excitations of key_in using the bit masks of holes and
|
||||
particles.
|
||||
Assume N_int is already provided.
|
||||
|
@ -1,5 +1,12 @@
|
||||
subroutine run_mrcc
|
||||
implicit none
|
||||
call set_generators_bitmasks_as_holes_and_particles
|
||||
call mrcc_iterations
|
||||
end
|
||||
|
||||
subroutine mrcc_iterations
|
||||
implicit none
|
||||
|
||||
integer :: i,j
|
||||
|
||||
double precision :: E_new, E_old, delta_e
|
||||
@ -24,7 +31,37 @@ subroutine run_mrcc
|
||||
call save_wavefunction
|
||||
enddo
|
||||
call write_double(6,ci_energy_dressed(1),"Final MRCC energy")
|
||||
call ezfio_set_mrcc_energy(ci_energy_dressed(1))
|
||||
call ezfio_set_mrcc_cassd_energy(ci_energy_dressed(1))
|
||||
call save_wavefunction
|
||||
|
||||
end
|
||||
|
||||
subroutine set_generators_bitmasks_as_holes_and_particles
|
||||
implicit none
|
||||
integer :: i,k
|
||||
do k = 1, N_generators_bitmask
|
||||
do i = 1, N_int
|
||||
! Pure single part
|
||||
generators_bitmask(i,1,1,k) = holes_operators(i,1) ! holes for pure single exc alpha
|
||||
generators_bitmask(i,1,2,k) = particles_operators(i,1) ! particles for pure single exc alpha
|
||||
generators_bitmask(i,2,1,k) = holes_operators(i,2) ! holes for pure single exc beta
|
||||
generators_bitmask(i,2,2,k) = particles_operators(i,2) ! particles for pure single exc beta
|
||||
|
||||
! Double excitation
|
||||
generators_bitmask(i,1,3,k) = holes_operators(i,1) ! holes for first single exc alpha
|
||||
generators_bitmask(i,1,4,k) = particles_operators(i,1) ! particles for first single exc alpha
|
||||
generators_bitmask(i,2,3,k) = holes_operators(i,2) ! holes for first single exc beta
|
||||
generators_bitmask(i,2,4,k) = particles_operators(i,2) ! particles for first single exc beta
|
||||
|
||||
generators_bitmask(i,1,5,k) = holes_operators(i,1) ! holes for second single exc alpha
|
||||
generators_bitmask(i,1,6,k) = particles_operators(i,1) ! particles for second single exc alpha
|
||||
generators_bitmask(i,2,5,k) = holes_operators(i,2) ! holes for second single exc beta
|
||||
generators_bitmask(i,2,6,k) = particles_operators(i,2) ! particles for second single exc beta
|
||||
|
||||
enddo
|
||||
enddo
|
||||
touch generators_bitmask
|
||||
|
||||
|
||||
|
||||
end
|
||||
|
@ -63,7 +63,7 @@ BEGIN_PROVIDER [ double precision, h_matrix_dressed, (N_det,N_det,N_states) ]
|
||||
i =idx_ref(ii)
|
||||
h_matrix_dressed(i,i,istate) += delta_ii(ii,istate)
|
||||
do jj = 1, N_det_non_ref
|
||||
j =idx_ref(jj)
|
||||
j =idx_non_ref(jj)
|
||||
h_matrix_dressed(i,j,istate) += delta_ij(ii,jj,istate)
|
||||
h_matrix_dressed(j,i,istate) += delta_ij(ii,jj,istate)
|
||||
enddo
|
||||
|
23
plugins/MRCC_Utils_new/README.rst
Normal file
@ -0,0 +1,23 @@
|
||||
===========
|
||||
MRCC Module
|
||||
===========
|
||||
|
||||
Needed Modules
|
||||
==============
|
||||
|
||||
.. Do not edit this section. It was auto-generated from the
|
||||
.. by the `update_README.py` script.
|
||||
|
||||
.. image:: tree_dependency.png
|
||||
|
||||
* `Perturbation <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation>`_
|
||||
* `Selectors_full <http://github.com/LCPQ/quantum_package/tree/master/src/Selectors_full>`_
|
||||
* `Generators_full <http://github.com/LCPQ/quantum_package/tree/master/src/Generators_full>`_
|
||||
* `Psiref_Utils <http://github.com/LCPQ/quantum_package/tree/master/src/Psiref_Utils>`_
|
||||
|
||||
Documentation
|
||||
=============
|
||||
|
||||
.. Do not edit this section. It was auto-generated from the
|
||||
.. by the `update_README.py` script.
|
||||
|
430
plugins/MRCC_Utils_new/davidson.irp.f
Normal file
@ -0,0 +1,430 @@
|
||||
subroutine davidson_diag_mrcc(dets_in,u_in,energies,dim_in,sze,N_st,Nint,iunit,istate)
|
||||
use bitmasks
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Davidson diagonalization.
|
||||
!
|
||||
! dets_in : bitmasks corresponding to determinants
|
||||
!
|
||||
! u_in : guess coefficients on the various states. Overwritten
|
||||
! on exit
|
||||
!
|
||||
! dim_in : leftmost dimension of u_in
|
||||
!
|
||||
! sze : Number of determinants
|
||||
!
|
||||
! N_st : Number of eigenstates
|
||||
!
|
||||
! iunit : Unit number for the I/O
|
||||
!
|
||||
! Initial guess vectors are not necessarily orthonormal
|
||||
END_DOC
|
||||
integer, intent(in) :: dim_in, sze, N_st, Nint, iunit, istate
|
||||
integer(bit_kind), intent(in) :: dets_in(Nint,2,sze)
|
||||
double precision, intent(inout) :: u_in(dim_in,N_st)
|
||||
double precision, intent(out) :: energies(N_st)
|
||||
double precision, allocatable :: H_jj(:)
|
||||
|
||||
double precision :: diag_h_mat_elem
|
||||
integer :: i
|
||||
ASSERT (N_st > 0)
|
||||
ASSERT (sze > 0)
|
||||
ASSERT (Nint > 0)
|
||||
ASSERT (Nint == N_int)
|
||||
PROVIDE mo_bielec_integrals_in_map
|
||||
allocate(H_jj(sze))
|
||||
|
||||
!$OMP PARALLEL DEFAULT(NONE) &
|
||||
!$OMP SHARED(sze,H_jj,N_det_ref,dets_in,Nint,istate,delta_ii,idx_ref) &
|
||||
!$OMP PRIVATE(i)
|
||||
!$OMP DO SCHEDULE(guided)
|
||||
do i=1,sze
|
||||
H_jj(i) = diag_h_mat_elem(dets_in(1,1,i),Nint)
|
||||
enddo
|
||||
!$OMP END DO
|
||||
!$OMP DO SCHEDULE(guided)
|
||||
do i=1,N_det_ref
|
||||
H_jj(idx_ref(i)) += delta_ii(i,istate)
|
||||
enddo
|
||||
!$OMP END DO
|
||||
!$OMP END PARALLEL
|
||||
|
||||
call davidson_diag_hjj_mrcc(dets_in,u_in,H_jj,energies,dim_in,sze,N_st,Nint,iunit,istate)
|
||||
deallocate (H_jj)
|
||||
end
|
||||
|
||||
subroutine davidson_diag_hjj_mrcc(dets_in,u_in,H_jj,energies,dim_in,sze,N_st,Nint,iunit,istate)
|
||||
use bitmasks
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Davidson diagonalization with specific diagonal elements of the H matrix
|
||||
!
|
||||
! H_jj : specific diagonal H matrix elements to diagonalize de Davidson
|
||||
!
|
||||
! dets_in : bitmasks corresponding to determinants
|
||||
!
|
||||
! u_in : guess coefficients on the various states. Overwritten
|
||||
! on exit
|
||||
!
|
||||
! dim_in : leftmost dimension of u_in
|
||||
!
|
||||
! sze : Number of determinants
|
||||
!
|
||||
! N_st : Number of eigenstates
|
||||
!
|
||||
! iunit : Unit for the I/O
|
||||
!
|
||||
! Initial guess vectors are not necessarily orthonormal
|
||||
END_DOC
|
||||
integer, intent(in) :: dim_in, sze, N_st, Nint, istate
|
||||
integer(bit_kind), intent(in) :: dets_in(Nint,2,sze)
|
||||
double precision, intent(in) :: H_jj(sze)
|
||||
integer, intent(in) :: iunit
|
||||
double precision, intent(inout) :: u_in(dim_in,N_st)
|
||||
double precision, intent(out) :: energies(N_st)
|
||||
|
||||
integer :: iter
|
||||
integer :: i,j,k,l,m
|
||||
logical :: converged
|
||||
|
||||
double precision :: overlap(N_st,N_st)
|
||||
double precision :: u_dot_v, u_dot_u
|
||||
|
||||
integer, allocatable :: kl_pairs(:,:)
|
||||
integer :: k_pairs, kl
|
||||
|
||||
integer :: iter2
|
||||
double precision, allocatable :: W(:,:,:), U(:,:,:), R(:,:)
|
||||
double precision, allocatable :: y(:,:,:,:), h(:,:,:,:), lambda(:)
|
||||
double precision :: diag_h_mat_elem
|
||||
double precision :: residual_norm(N_st)
|
||||
character*(16384) :: write_buffer
|
||||
double precision :: to_print(2,N_st)
|
||||
double precision :: cpu, wall
|
||||
|
||||
PROVIDE det_connections
|
||||
|
||||
call write_time(iunit)
|
||||
call wall_time(wall)
|
||||
call cpu_time(cpu)
|
||||
write(iunit,'(A)') ''
|
||||
write(iunit,'(A)') 'Davidson Diagonalization'
|
||||
write(iunit,'(A)') '------------------------'
|
||||
write(iunit,'(A)') ''
|
||||
call write_int(iunit,N_st,'Number of states')
|
||||
call write_int(iunit,sze,'Number of determinants')
|
||||
write(iunit,'(A)') ''
|
||||
write_buffer = '===== '
|
||||
do i=1,N_st
|
||||
write_buffer = trim(write_buffer)//' ================ ================'
|
||||
enddo
|
||||
write(iunit,'(A)') trim(write_buffer)
|
||||
write_buffer = ' Iter'
|
||||
do i=1,N_st
|
||||
write_buffer = trim(write_buffer)//' Energy Residual'
|
||||
enddo
|
||||
write(iunit,'(A)') trim(write_buffer)
|
||||
write_buffer = '===== '
|
||||
do i=1,N_st
|
||||
write_buffer = trim(write_buffer)//' ================ ================'
|
||||
enddo
|
||||
write(iunit,'(A)') trim(write_buffer)
|
||||
|
||||
allocate( &
|
||||
kl_pairs(2,N_st*(N_st+1)/2), &
|
||||
W(sze,N_st,davidson_sze_max), &
|
||||
U(sze,N_st,davidson_sze_max), &
|
||||
R(sze,N_st), &
|
||||
h(N_st,davidson_sze_max,N_st,davidson_sze_max), &
|
||||
y(N_st,davidson_sze_max,N_st,davidson_sze_max), &
|
||||
lambda(N_st*davidson_sze_max))
|
||||
|
||||
ASSERT (N_st > 0)
|
||||
ASSERT (sze > 0)
|
||||
ASSERT (Nint > 0)
|
||||
ASSERT (Nint == N_int)
|
||||
|
||||
! Initialization
|
||||
! ==============
|
||||
|
||||
k_pairs=0
|
||||
do l=1,N_st
|
||||
do k=1,l
|
||||
k_pairs+=1
|
||||
kl_pairs(1,k_pairs) = k
|
||||
kl_pairs(2,k_pairs) = l
|
||||
enddo
|
||||
enddo
|
||||
|
||||
!$OMP PARALLEL DEFAULT(NONE) &
|
||||
!$OMP SHARED(U,sze,N_st,overlap,kl_pairs,k_pairs, &
|
||||
!$OMP Nint,dets_in,u_in) &
|
||||
!$OMP PRIVATE(k,l,kl,i)
|
||||
|
||||
|
||||
! Orthonormalize initial guess
|
||||
! ============================
|
||||
|
||||
!$OMP DO
|
||||
do kl=1,k_pairs
|
||||
k = kl_pairs(1,kl)
|
||||
l = kl_pairs(2,kl)
|
||||
if (k/=l) then
|
||||
overlap(k,l) = u_dot_v(U_in(1,k),U_in(1,l),sze)
|
||||
overlap(l,k) = overlap(k,l)
|
||||
else
|
||||
overlap(k,k) = u_dot_u(U_in(1,k),sze)
|
||||
endif
|
||||
enddo
|
||||
!$OMP END DO
|
||||
!$OMP END PARALLEL
|
||||
|
||||
call ortho_lowdin(overlap,size(overlap,1),N_st,U_in,size(U_in,1),sze)
|
||||
|
||||
! Davidson iterations
|
||||
! ===================
|
||||
|
||||
converged = .False.
|
||||
|
||||
do while (.not.converged)
|
||||
|
||||
!$OMP PARALLEL DEFAULT(NONE) &
|
||||
!$OMP PRIVATE(k,i) SHARED(U,u_in,sze,N_st)
|
||||
do k=1,N_st
|
||||
!$OMP DO
|
||||
do i=1,sze
|
||||
U(i,k,1) = u_in(i,k)
|
||||
enddo
|
||||
!$OMP END DO
|
||||
enddo
|
||||
!$OMP END PARALLEL
|
||||
|
||||
do iter=1,davidson_sze_max-1
|
||||
|
||||
! Compute W_k = H |u_k>
|
||||
! ----------------------
|
||||
|
||||
do k=1,N_st
|
||||
call H_u_0_mrcc(W(1,k,iter),U(1,k,iter),H_jj,sze,dets_in,Nint,istate)
|
||||
enddo
|
||||
|
||||
! Compute h_kl = <u_k | W_l> = <u_k| H |u_l>
|
||||
! -------------------------------------------
|
||||
|
||||
do l=1,N_st
|
||||
do k=1,N_st
|
||||
do iter2=1,iter-1
|
||||
h(k,iter2,l,iter) = u_dot_v(U(1,k,iter2),W(1,l,iter),sze)
|
||||
h(k,iter,l,iter2) = h(k,iter2,l,iter)
|
||||
enddo
|
||||
enddo
|
||||
do k=1,l
|
||||
h(k,iter,l,iter) = u_dot_v(U(1,k,iter),W(1,l,iter),sze)
|
||||
h(l,iter,k,iter) = h(k,iter,l,iter)
|
||||
enddo
|
||||
enddo
|
||||
|
||||
!DEBUG H MATRIX
|
||||
!do i=1,iter
|
||||
! print '(10(x,F16.10))', h(1,i,1,1:i)
|
||||
!enddo
|
||||
!print *, ''
|
||||
!END
|
||||
|
||||
! Diagonalize h
|
||||
! -------------
|
||||
call lapack_diag(lambda,y,h,N_st*davidson_sze_max,N_st*iter)
|
||||
|
||||
! Express eigenvectors of h in the determinant basis
|
||||
! --------------------------------------------------
|
||||
|
||||
do k=1,N_st
|
||||
do i=1,sze
|
||||
U(i,k,iter+1) = 0.d0
|
||||
W(i,k,iter+1) = 0.d0
|
||||
do l=1,N_st
|
||||
do iter2=1,iter
|
||||
U(i,k,iter+1) = U(i,k,iter+1) + U(i,l,iter2)*y(l,iter2,k,1)
|
||||
W(i,k,iter+1) = W(i,k,iter+1) + W(i,l,iter2)*y(l,iter2,k,1)
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
|
||||
! Compute residual vector
|
||||
! -----------------------
|
||||
|
||||
do k=1,N_st
|
||||
do i=1,sze
|
||||
R(i,k) = lambda(k) * U(i,k,iter+1) - W(i,k,iter+1)
|
||||
enddo
|
||||
residual_norm(k) = u_dot_u(R(1,k),sze)
|
||||
to_print(1,k) = lambda(k) + nuclear_repulsion
|
||||
to_print(2,k) = residual_norm(k)
|
||||
enddo
|
||||
|
||||
write(iunit,'(X,I3,X,100(X,F16.10,X,E16.6))'), iter, to_print(:,1:N_st)
|
||||
call davidson_converged(lambda,residual_norm,wall,iter,cpu,N_st,converged)
|
||||
if (converged) then
|
||||
exit
|
||||
endif
|
||||
|
||||
|
||||
! Davidson step
|
||||
! -------------
|
||||
|
||||
do k=1,N_st
|
||||
do i=1,sze
|
||||
U(i,k,iter+1) = -1.d0/max(H_jj(i) - lambda(k),1.d-2) * R(i,k)
|
||||
enddo
|
||||
enddo
|
||||
|
||||
! Gram-Schmidt
|
||||
! ------------
|
||||
|
||||
double precision :: c
|
||||
do k=1,N_st
|
||||
do iter2=1,iter
|
||||
do l=1,N_st
|
||||
c = u_dot_v(U(1,k,iter+1),U(1,l,iter2),sze)
|
||||
do i=1,sze
|
||||
U(i,k,iter+1) -= c * U(i,l,iter2)
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
do l=1,k-1
|
||||
c = u_dot_v(U(1,k,iter+1),U(1,l,iter+1),sze)
|
||||
do i=1,sze
|
||||
U(i,k,iter+1) -= c * U(i,l,iter+1)
|
||||
enddo
|
||||
enddo
|
||||
call normalize( U(1,k,iter+1), sze )
|
||||
enddo
|
||||
|
||||
!DEBUG : CHECK OVERLAP
|
||||
!print *, '==='
|
||||
!do k=1,iter+1
|
||||
! do l=1,k
|
||||
! c = u_dot_v(U(1,1,k),U(1,1,l),sze)
|
||||
! print *, k,l, c
|
||||
! enddo
|
||||
!enddo
|
||||
!print *, '==='
|
||||
!pause
|
||||
!END DEBUG
|
||||
|
||||
|
||||
enddo
|
||||
|
||||
if (.not.converged) then
|
||||
iter = davidson_sze_max-1
|
||||
endif
|
||||
|
||||
! Re-contract to u_in
|
||||
! -----------
|
||||
|
||||
do k=1,N_st
|
||||
energies(k) = lambda(k)
|
||||
do i=1,sze
|
||||
u_in(i,k) = 0.d0
|
||||
do iter2=1,iter
|
||||
do l=1,N_st
|
||||
u_in(i,k) += U(i,l,iter2)*y(l,iter2,k,1)
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
|
||||
enddo
|
||||
|
||||
write_buffer = '===== '
|
||||
do i=1,N_st
|
||||
write_buffer = trim(write_buffer)//' ================ ================'
|
||||
enddo
|
||||
write(iunit,'(A)') trim(write_buffer)
|
||||
write(iunit,'(A)') ''
|
||||
call write_time(iunit)
|
||||
|
||||
deallocate ( &
|
||||
kl_pairs, &
|
||||
W, &
|
||||
U, &
|
||||
R, &
|
||||
h, &
|
||||
y, &
|
||||
lambda &
|
||||
)
|
||||
abort_here = abort_all
|
||||
end
|
||||
|
||||
subroutine H_u_0_mrcc(v_0,u_0,H_jj,n,keys_tmp,Nint,istate)
|
||||
use bitmasks
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Computes v_0 = H|u_0>
|
||||
!
|
||||
! n : number of determinants
|
||||
!
|
||||
! H_jj : array of <j|H|j>
|
||||
END_DOC
|
||||
integer, intent(in) :: n,Nint,istate
|
||||
double precision, intent(out) :: v_0(n)
|
||||
double precision, intent(in) :: u_0(n)
|
||||
double precision, intent(in) :: H_jj(n)
|
||||
integer(bit_kind),intent(in) :: keys_tmp(Nint,2,n)
|
||||
integer, allocatable :: idx(:)
|
||||
double precision :: hij
|
||||
double precision, allocatable :: vt(:)
|
||||
integer :: i,j,k,l, jj,ii
|
||||
integer :: i0, j0
|
||||
ASSERT (Nint > 0)
|
||||
ASSERT (Nint == N_int)
|
||||
ASSERT (n>0)
|
||||
PROVIDE ref_bitmask_energy delta_ij
|
||||
integer, parameter :: block_size = 157
|
||||
!$OMP PARALLEL DEFAULT(NONE) &
|
||||
!$OMP PRIVATE(i,hij,j,k,idx,jj,ii,vt) &
|
||||
!$OMP SHARED(n_det_ref,n_det_non_ref,idx_ref,idx_non_ref,n,H_jj,u_0,keys_tmp,Nint,v_0,istate,delta_ij)
|
||||
!$OMP DO SCHEDULE(static)
|
||||
do i=1,n
|
||||
v_0(i) = H_jj(i) * u_0(i)
|
||||
enddo
|
||||
!$OMP END DO
|
||||
allocate(idx(0:n), vt(n))
|
||||
Vt = 0.d0
|
||||
!$OMP DO SCHEDULE(guided)
|
||||
do i=1,n
|
||||
idx(0) = i
|
||||
call filter_connected_davidson(keys_tmp,keys_tmp(1,1,i),Nint,i-1,idx)
|
||||
do jj=1,idx(0)
|
||||
j = idx(jj)
|
||||
if ( (dabs(u_0(j)) > 1.d-7).or.((dabs(u_0(i)) > 1.d-7)) ) then
|
||||
call i_H_j(keys_tmp(1,1,j),keys_tmp(1,1,i),Nint,hij)
|
||||
hij = hij
|
||||
vt (i) = vt (i) + hij*u_0(j)
|
||||
vt (j) = vt (j) + hij*u_0(i)
|
||||
endif
|
||||
enddo
|
||||
enddo
|
||||
!$OMP END DO
|
||||
|
||||
!$OMP DO SCHEDULE(guided)
|
||||
do ii=1,n_det_ref
|
||||
i = idx_ref(ii)
|
||||
do jj = 1, n_det_non_ref
|
||||
j = idx_non_ref(jj)
|
||||
vt (i) = vt (i) + delta_ij(ii,jj,istate)*u_0(j)
|
||||
vt (j) = vt (j) + delta_ij(ii,jj,istate)*u_0(i)
|
||||
enddo
|
||||
enddo
|
||||
!$OMP END DO
|
||||
!$OMP CRITICAL
|
||||
do i=1,n
|
||||
v_0(i) = v_0(i) + vt(i)
|
||||
enddo
|
||||
!$OMP END CRITICAL
|
||||
deallocate(idx,vt)
|
||||
!$OMP END PARALLEL
|
||||
end
|
||||
|
||||
|
85
plugins/MRCC_Utils_new/mrcc_amplitudes.irp.f
Normal file
@ -0,0 +1,85 @@
|
||||
subroutine get_excitation_operators_for_one_ref(det_ref,i_state,ndetnonref,N_connect_ref,excitation_operators,amplitudes_phase_less,index_connected)
|
||||
use bitmasks
|
||||
implicit none
|
||||
integer(bit_kind), intent(in) :: det_ref(N_int,2)
|
||||
integer, intent(in) :: i_state,ndetnonref
|
||||
integer*2, intent(out) :: excitation_operators(5,ndetnonref)
|
||||
integer, intent(out) :: index_connected(ndetnonref)
|
||||
integer, intent(out) :: N_connect_ref
|
||||
double precision, intent(out) :: amplitudes_phase_less(ndetnonref)
|
||||
|
||||
integer :: i,j,k,l,degree,h1,p1,h2,p2,s1,s2
|
||||
integer :: exc(0:2,2,2)
|
||||
double precision :: phase,hij
|
||||
BEGIN_DOC
|
||||
! This subroutine provides all the amplitudes and excitation operators
|
||||
! that one needs to go from the reference to the non reference wave function
|
||||
! you enter with det_ref that is a reference determinant
|
||||
!
|
||||
! N_connect_ref is the number of determinants belonging to psi_non_ref
|
||||
! that are connected to det_ref.
|
||||
!
|
||||
! amplitudes_phase_less(i) = amplitude phase less t_{I->i} = <I|H|i> * lambda_mrcc(i) * phase(I->i)
|
||||
!
|
||||
! excitation_operators(:,i) represents the holes and particles that
|
||||
! link the ith connected determinant to det_ref
|
||||
! if ::
|
||||
! excitation_operators(5,i) = 2 :: double excitation alpha
|
||||
! excitation_operators(5,i) = -2 :: double excitation beta
|
||||
!!! excitation_operators(1,i) :: hole 1
|
||||
!!! excitation_operators(2,i) :: particle 1
|
||||
!!! excitation_operators(3,i) :: hole 2
|
||||
!!! excitation_operators(4,i) :: particle 2
|
||||
! else if ::
|
||||
! excitation_operators(5,i) = 1 :: single excitation alpha
|
||||
!!! excitation_operators(1,i) :: hole 1
|
||||
!!! excitation_operators(2,i) :: particle 1
|
||||
! else if ::
|
||||
! excitation_operators(5,i) = -1 :: single excitation beta
|
||||
!!! excitation_operators(3,i) :: hole 1
|
||||
!!! excitation_operators(4,i) :: particle 1
|
||||
! else if ::
|
||||
!!! excitation_operators(5,i) = 0 :: double excitation alpha/beta
|
||||
!!! excitation_operators(1,i) :: hole 1 alpha
|
||||
!!! excitation_operators(2,i) :: particle 1 alpha
|
||||
!!! excitation_operators(3,i) :: hole 2 beta
|
||||
!!! excitation_operators(4,i) :: particle 2 beta
|
||||
END_DOC
|
||||
N_connect_ref = 0
|
||||
do i = 1, ndetnonref
|
||||
call i_H_j_phase_out(det_ref,psi_non_ref(1,1,i),N_int,hij,phase,exc,degree)
|
||||
! if(dabs(hij).le.mo_integrals_threshold)cycle
|
||||
N_connect_ref +=1
|
||||
index_connected(N_connect_ref) = i
|
||||
call decode_exc(exc,degree,h1,p1,h2,p2,s1,s2)
|
||||
amplitudes_phase_less(N_connect_ref) = hij * lambda_mrcc(i_state,i) !*phase
|
||||
|
||||
if(degree==2)then
|
||||
excitation_operators(1,N_connect_ref) = h1
|
||||
excitation_operators(2,N_connect_ref) = p1
|
||||
excitation_operators(3,N_connect_ref) = h2
|
||||
excitation_operators(4,N_connect_ref) = p2
|
||||
if(s1==s2.and.s1==1)then ! double alpha
|
||||
excitation_operators(5,N_connect_ref)= 2
|
||||
elseif(s1==s2.and.s1==2)then ! double beta
|
||||
excitation_operators(5,N_connect_ref)=-2
|
||||
else
|
||||
excitation_operators(5,N_connect_ref)= 0 ! double alpha/beta
|
||||
endif
|
||||
elseif(degree==1)then
|
||||
if(s1==1)then ! mono alpha
|
||||
excitation_operators(5,N_connect_ref)= 1
|
||||
excitation_operators(1,N_connect_ref) = h1
|
||||
excitation_operators(2,N_connect_ref) = p1
|
||||
else ! mono beta
|
||||
excitation_operators(5,N_connect_ref)=-1
|
||||
excitation_operators(3,N_connect_ref) = h1
|
||||
excitation_operators(4,N_connect_ref) = p1
|
||||
endif
|
||||
else
|
||||
N_connect_ref-=1
|
||||
endif
|
||||
|
||||
enddo
|
||||
|
||||
end
|
129
plugins/MRCC_Utils_new/mrcc_dress.irp.f
Normal file
@ -0,0 +1,129 @@
|
||||
subroutine mrcc_dress(ndetref,ndetnonref,nstates,delta_ij_,delta_ii_)
|
||||
use bitmasks
|
||||
implicit none
|
||||
integer, intent(in) :: ndetref,nstates,ndetnonref
|
||||
double precision, intent(inout) :: delta_ii_(ndetref,nstates),delta_ij_(ndetref,ndetnonref,nstates)
|
||||
integer :: i,j,k,l
|
||||
integer :: i_state
|
||||
integer :: N_connect_ref
|
||||
integer*2,allocatable :: excitation_operators(:,:)
|
||||
double precision, allocatable :: amplitudes_phase_less(:)
|
||||
double precision, allocatable :: coef_test(:)
|
||||
integer(bit_kind), allocatable :: key_test(:,:)
|
||||
integer, allocatable :: index_connected(:)
|
||||
integer :: i_hole,i_particle,ispin,i_ok,connected_to_ref,index_wf
|
||||
integer, allocatable :: idx_vector(:), degree_vector(:)
|
||||
double precision :: phase_ij
|
||||
double precision :: dij,phase_la
|
||||
double precision :: hij,phase
|
||||
integer :: exc(0:2,2,2),degree
|
||||
logical :: is_in_wavefunction
|
||||
allocate(excitation_operators(5,N_det_non_ref))
|
||||
allocate(amplitudes_phase_less(N_det_non_ref))
|
||||
allocate(key_test(N_int,2))
|
||||
allocate(index_connected(N_det_non_ref))
|
||||
allocate(idx_vector(0:N_det_non_ref))
|
||||
allocate(degree_vector(N_det_non_ref))
|
||||
i_state = 1
|
||||
|
||||
do i = 1, N_det_ref
|
||||
call get_excitation_operators_for_one_ref(psi_ref(1,1,i),i_state,N_det_non_ref,N_connect_ref,excitation_operators,amplitudes_phase_less,index_connected)
|
||||
print*,'N_connect_ref =',N_connect_ref
|
||||
do l = 1, N_det_non_ref
|
||||
double precision :: t_il,phase_il,hil
|
||||
call i_H_j_phase_out(psi_ref(1,1,i),psi_non_ref(1,1,l),N_int,hil,phase_il,exc,degree)
|
||||
t_il = hil * lambda_mrcc(i_state,l)
|
||||
! loop on the non ref determinants
|
||||
do j = 1, N_connect_ref
|
||||
! loop on the excitation operators linked to i
|
||||
if(j==l)cycle
|
||||
do k = 1, N_int
|
||||
key_test(k,1) = psi_non_ref(k,1,l)
|
||||
key_test(k,2) = psi_non_ref(k,2,l)
|
||||
enddo
|
||||
! we apply the excitation operator T_I->j
|
||||
call apply_excitation_operator(key_test,excitation_operators(1,j),i_ok)
|
||||
if(i_ok.ne.1)cycle
|
||||
! we check if such determinant is already in the wave function
|
||||
if(is_in_wavefunction(key_test,N_int,N_det))cycle
|
||||
! we get the phase for psi_non_ref(l) -> T_I->j |psi_non_ref(l)>
|
||||
call get_excitation(psi_non_ref(1,1,l),key_test,exc,degree,phase_la,N_int)
|
||||
! we get the phase T_I->j
|
||||
call i_H_j_phase_out(psi_ref(1,1,i),psi_non_ref(1,1,index_connected(j)),N_int,hij,phase_ij,exc,degree)
|
||||
! we compute the contribution to the coef of key_test
|
||||
dij = t_il * hij * phase_la *phase_ij *lambda_mrcc(i_state,index_connected(j)) * 0.5d0
|
||||
! we compute the interaction of such determinant with all the non_ref dets
|
||||
call get_excitation_degree_vector(psi_non_ref,key_test,degree_vector,N_int,N_det_non_ref,idx_vector)
|
||||
do k = 1, idx_vector(0)
|
||||
call i_H_j_phase_out(key_test,psi_non_ref(1,1,idx_vector(k)),N_int,hij,phase,exc,degree)
|
||||
delta_ij_(i,idx_vector(k),i_state) += hij * dij
|
||||
enddo
|
||||
enddo
|
||||
if(dabs(psi_ref_coef(i,i_state)).le.5.d-5)cycle
|
||||
! delta_ij_(i,l,i_state) = delta_ij_(i,l,i_state) * 0.5d0
|
||||
delta_ii_(i,i_state) -= delta_ij_(i,l,i_state) * psi_non_ref_coef(l,i_state) / psi_ref_coef(i,i_state)
|
||||
enddo
|
||||
enddo
|
||||
|
||||
deallocate(excitation_operators)
|
||||
deallocate(amplitudes_phase_less)
|
||||
deallocate(key_test)
|
||||
deallocate(idx_vector)
|
||||
deallocate(degree_vector)
|
||||
|
||||
end
|
||||
|
||||
|
||||
|
||||
subroutine apply_excitation_operator(key_in,excitation_operator,i_ok)
|
||||
use bitmasks
|
||||
implicit none
|
||||
integer(bit_kind), intent(inout) :: key_in
|
||||
integer, intent (out) :: i_ok
|
||||
integer*2 :: excitation_operator(5)
|
||||
integer :: i_particle,i_hole,ispin
|
||||
! Do excitation
|
||||
if(excitation_operator(5)==1)then ! mono alpha
|
||||
i_hole = excitation_operator(1)
|
||||
i_particle = excitation_operator(2)
|
||||
ispin = 1
|
||||
call do_mono_excitation(key_in,i_hole,i_particle,ispin,i_ok)
|
||||
else if (excitation_operator(5)==-1)then ! mono beta
|
||||
i_hole = excitation_operator(3)
|
||||
i_particle = excitation_operator(4)
|
||||
ispin = 2
|
||||
call do_mono_excitation(key_in,i_hole,i_particle,ispin,i_ok)
|
||||
else if (excitation_operator(5) == -2 )then ! double beta
|
||||
i_hole = excitation_operator(1)
|
||||
i_particle = excitation_operator(2)
|
||||
ispin = 2
|
||||
call do_mono_excitation(key_in,i_hole,i_particle,ispin,i_ok)
|
||||
if(i_ok.ne.1)return
|
||||
i_hole = excitation_operator(3)
|
||||
i_particle = excitation_operator(4)
|
||||
ispin = 2
|
||||
call do_mono_excitation(key_in,i_hole,i_particle,ispin,i_ok)
|
||||
|
||||
else if (excitation_operator(5) == 2 )then ! double alpha
|
||||
i_hole = excitation_operator(1)
|
||||
i_particle = excitation_operator(2)
|
||||
ispin = 1
|
||||
call do_mono_excitation(key_in,i_hole,i_particle,ispin,i_ok)
|
||||
if(i_ok.ne.1)return
|
||||
i_hole = excitation_operator(3)
|
||||
i_particle = excitation_operator(4)
|
||||
ispin = 1
|
||||
call do_mono_excitation(key_in,i_hole,i_particle,ispin,i_ok)
|
||||
|
||||
else if (excitation_operator(5) == 0 )then ! double alpha/alpha
|
||||
i_hole = excitation_operator(1)
|
||||
i_particle = excitation_operator(2)
|
||||
ispin = 1
|
||||
call do_mono_excitation(key_in,i_hole,i_particle,ispin,i_ok)
|
||||
if(i_ok.ne.1)return
|
||||
i_hole = excitation_operator(3)
|
||||
i_particle = excitation_operator(4)
|
||||
ispin = 2
|
||||
call do_mono_excitation(key_in,i_hole,i_particle,ispin,i_ok)
|
||||
endif
|
||||
end
|
67
plugins/MRCC_Utils_new/mrcc_general.irp.f
Normal file
@ -0,0 +1,67 @@
|
||||
subroutine run_mrcc
|
||||
implicit none
|
||||
call set_generators_bitmasks_as_holes_and_particles
|
||||
call mrcc_iterations
|
||||
end
|
||||
|
||||
subroutine mrcc_iterations
|
||||
implicit none
|
||||
|
||||
integer :: i,j
|
||||
|
||||
double precision :: E_new, E_old, delta_e
|
||||
integer :: iteration
|
||||
E_new = 0.d0
|
||||
delta_E = 1.d0
|
||||
iteration = 0
|
||||
do while (delta_E > 1.d-8)
|
||||
iteration += 1
|
||||
print *, '==========================='
|
||||
print *, 'MRCC Iteration', iteration
|
||||
print *, '==========================='
|
||||
print *, ''
|
||||
E_old = sum(ci_energy_dressed)
|
||||
call write_double(6,ci_energy_dressed(1),"MRCC energy")
|
||||
call diagonalize_ci_dressed
|
||||
E_new = sum(ci_energy_dressed)
|
||||
delta_E = dabs(E_new - E_old)
|
||||
! stop
|
||||
if (iteration > 200) then
|
||||
exit
|
||||
endif
|
||||
enddo
|
||||
call write_double(6,ci_energy_dressed(1),"Final MRCC energy")
|
||||
call ezfio_set_mrcc_cassd_energy(ci_energy_dressed(1))
|
||||
call save_wavefunction
|
||||
|
||||
end
|
||||
|
||||
subroutine set_generators_bitmasks_as_holes_and_particles
|
||||
implicit none
|
||||
integer :: i,k
|
||||
do k = 1, N_generators_bitmask
|
||||
do i = 1, N_int
|
||||
! Pure single part
|
||||
generators_bitmask(i,1,1,k) = holes_operators(i,1) ! holes for pure single exc alpha
|
||||
generators_bitmask(i,1,2,k) = particles_operators(i,1) ! particles for pure single exc alpha
|
||||
generators_bitmask(i,2,1,k) = holes_operators(i,2) ! holes for pure single exc beta
|
||||
generators_bitmask(i,2,2,k) = particles_operators(i,2) ! particles for pure single exc beta
|
||||
|
||||
! Double excitation
|
||||
generators_bitmask(i,1,3,k) = holes_operators(i,1) ! holes for first single exc alpha
|
||||
generators_bitmask(i,1,4,k) = particles_operators(i,1) ! particles for first single exc alpha
|
||||
generators_bitmask(i,2,3,k) = holes_operators(i,2) ! holes for first single exc beta
|
||||
generators_bitmask(i,2,4,k) = particles_operators(i,2) ! particles for first single exc beta
|
||||
|
||||
generators_bitmask(i,1,5,k) = holes_operators(i,1) ! holes for second single exc alpha
|
||||
generators_bitmask(i,1,6,k) = particles_operators(i,1) ! particles for second single exc alpha
|
||||
generators_bitmask(i,2,5,k) = holes_operators(i,2) ! holes for second single exc beta
|
||||
generators_bitmask(i,2,6,k) = particles_operators(i,2) ! particles for second single exc beta
|
||||
|
||||
enddo
|
||||
enddo
|
||||
touch generators_bitmask
|
||||
|
||||
|
||||
|
||||
end
|
179
plugins/MRCC_Utils_new/mrcc_utils.irp.f
Normal file
@ -0,0 +1,179 @@
|
||||
BEGIN_PROVIDER [ double precision, lambda_mrcc, (N_states,psi_det_size) ]
|
||||
&BEGIN_PROVIDER [ double precision, lambda_pert, (N_states,psi_det_size) ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! cm/<Psi_0|H|D_m> or perturbative 1/Delta_E(m)
|
||||
END_DOC
|
||||
integer :: i,k
|
||||
double precision :: ihpsi(N_states), hii
|
||||
integer :: i_ok
|
||||
i_ok = 0
|
||||
|
||||
do i=1,N_det_non_ref
|
||||
call i_h_psi(psi_non_ref(1,1,i), psi_ref, psi_ref_coef, N_int, N_det_ref,&
|
||||
size(psi_ref_coef,1), n_states, ihpsi)
|
||||
call i_h_j(psi_non_ref(1,1,i),psi_non_ref(1,1,i),N_int,hii)
|
||||
do k=1,N_states
|
||||
lambda_pert(k,i) = 1.d0 / (psi_ref_energy_diagonalized(k)-hii)
|
||||
if (dabs(ihpsi(k)).le.1.d-3) then
|
||||
i_ok +=1
|
||||
lambda_mrcc(k,i) = lambda_pert(k,i)
|
||||
else
|
||||
lambda_mrcc(k,i) = psi_non_ref_coef(i,k)/ihpsi(k)
|
||||
endif
|
||||
enddo
|
||||
enddo
|
||||
print*,'N_det_non_ref = ',N_det_non_ref
|
||||
print*,'Number of Perturbatively treated determinants = ',i_ok
|
||||
print*,'psi_coef_ref_ratio = ',psi_ref_coef(2,1)/psi_ref_coef(1,1)
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
|
||||
|
||||
|
||||
!BEGIN_PROVIDER [ double precision, delta_ij_non_ref, (N_det_non_ref, N_det_non_ref,N_states) ]
|
||||
!implicit none
|
||||
!BEGIN_DOC
|
||||
!! Dressing matrix in SD basis
|
||||
!END_DOC
|
||||
!delta_ij_non_ref = 0.d0
|
||||
!call H_apply_mrcc_simple(delta_ij_non_ref,N_det_non_ref)
|
||||
!END_PROVIDER
|
||||
|
||||
BEGIN_PROVIDER [ double precision, delta_ij, (N_det_ref,N_det_non_ref,N_states) ]
|
||||
&BEGIN_PROVIDER [ double precision, delta_ii, (N_det_ref,N_states) ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Dressing matrix in N_det basis
|
||||
END_DOC
|
||||
integer :: i,j,m
|
||||
delta_ij = 0.d0
|
||||
delta_ii = 0.d0
|
||||
call mrcc_dress(N_det_ref,N_det_non_ref,N_states,delta_ij,delta_ii)
|
||||
write(33,*)delta_ij
|
||||
write(34,*)delta_ii
|
||||
END_PROVIDER
|
||||
|
||||
BEGIN_PROVIDER [ double precision, h_matrix_dressed, (N_det,N_det,N_states) ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Dressed H with Delta_ij
|
||||
END_DOC
|
||||
integer :: i, j,istate,ii,jj
|
||||
do istate = 1,N_states
|
||||
do j=1,N_det
|
||||
do i=1,N_det
|
||||
h_matrix_dressed(i,j,istate) = h_matrix_all_dets(i,j)
|
||||
enddo
|
||||
enddo
|
||||
do ii = 1, N_det_ref
|
||||
i =idx_ref(ii)
|
||||
h_matrix_dressed(i,i,istate) += delta_ii(ii,istate)
|
||||
do jj = 1, N_det_non_ref
|
||||
j =idx_non_ref(jj)
|
||||
h_matrix_dressed(i,j,istate) += delta_ij(ii,jj,istate)
|
||||
h_matrix_dressed(j,i,istate) += delta_ij(ii,jj,istate)
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
END_PROVIDER
|
||||
|
||||
|
||||
BEGIN_PROVIDER [ double precision, CI_electronic_energy_dressed, (N_states_diag) ]
|
||||
&BEGIN_PROVIDER [ double precision, CI_eigenvectors_dressed, (N_det,N_states_diag) ]
|
||||
&BEGIN_PROVIDER [ double precision, CI_eigenvectors_s2_dressed, (N_states_diag) ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Eigenvectors/values of the CI matrix
|
||||
END_DOC
|
||||
integer :: i,j
|
||||
|
||||
do j=1,N_states_diag
|
||||
do i=1,N_det
|
||||
CI_eigenvectors_dressed(i,j) = psi_coef(i,j)
|
||||
enddo
|
||||
enddo
|
||||
|
||||
if (diag_algorithm == "Davidson") then
|
||||
|
||||
integer :: istate
|
||||
istate = 1
|
||||
call davidson_diag_mrcc(psi_det,CI_eigenvectors_dressed,CI_electronic_energy_dressed,&
|
||||
size(CI_eigenvectors_dressed,1),N_det,N_states_diag,N_int,output_determinants,istate)
|
||||
|
||||
else if (diag_algorithm == "Lapack") then
|
||||
|
||||
double precision, allocatable :: eigenvectors(:,:), eigenvalues(:)
|
||||
allocate (eigenvectors(size(H_matrix_dressed,1),N_det))
|
||||
allocate (eigenvalues(N_det))
|
||||
call lapack_diag(eigenvalues,eigenvectors, &
|
||||
H_matrix_dressed,size(H_matrix_dressed,1),N_det)
|
||||
CI_electronic_energy_dressed(:) = 0.d0
|
||||
do i=1,N_det
|
||||
CI_eigenvectors_dressed(i,1) = eigenvectors(i,1)
|
||||
enddo
|
||||
integer :: i_state
|
||||
double precision :: s2
|
||||
i_state = 0
|
||||
if (s2_eig) then
|
||||
do j=1,N_det
|
||||
call get_s2_u0(psi_det,eigenvectors(1,j),N_det,N_det,s2)
|
||||
if(dabs(s2-expected_s2).le.0.3d0)then
|
||||
i_state += 1
|
||||
do i=1,N_det
|
||||
CI_eigenvectors_dressed(i,i_state) = eigenvectors(i,j)
|
||||
enddo
|
||||
CI_electronic_energy_dressed(i_state) = eigenvalues(j)
|
||||
CI_eigenvectors_s2_dressed(i_state) = s2
|
||||
endif
|
||||
if (i_state.ge.N_states_diag) then
|
||||
exit
|
||||
endif
|
||||
enddo
|
||||
else
|
||||
do j=1,N_states_diag
|
||||
call get_s2_u0(psi_det,eigenvectors(1,j),N_det,N_det,s2)
|
||||
i_state += 1
|
||||
do i=1,N_det
|
||||
CI_eigenvectors_dressed(i,i_state) = eigenvectors(i,j)
|
||||
enddo
|
||||
CI_electronic_energy_dressed(i_state) = eigenvalues(j)
|
||||
CI_eigenvectors_s2_dressed(i_state) = s2
|
||||
enddo
|
||||
endif
|
||||
deallocate(eigenvectors,eigenvalues)
|
||||
endif
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
BEGIN_PROVIDER [ double precision, CI_energy_dressed, (N_states_diag) ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! N_states lowest eigenvalues of the dressed CI matrix
|
||||
END_DOC
|
||||
|
||||
integer :: j
|
||||
character*(8) :: st
|
||||
call write_time(output_determinants)
|
||||
do j=1,N_states_diag
|
||||
CI_energy_dressed(j) = CI_electronic_energy_dressed(j) + nuclear_repulsion
|
||||
enddo
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
subroutine diagonalize_CI_dressed
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Replace the coefficients of the CI states by the coefficients of the
|
||||
! eigenstates of the CI matrix
|
||||
END_DOC
|
||||
integer :: i,j
|
||||
do j=1,N_states_diag
|
||||
do i=1,N_det
|
||||
psi_coef(i,j) = CI_eigenvectors_dressed(i,j)
|
||||
enddo
|
||||
enddo
|
||||
SOFT_TOUCH psi_coef
|
||||
|
||||
end
|
BIN
plugins/MRCC_Utils_new/tree_dependency.png
Normal file
After Width: | Height: | Size: 106 KiB |
26
plugins/Molden/.gitignore
vendored
@ -1,18 +1,18 @@
|
||||
# Automatically created by /home/giner/quantum_package/scripts/module/module_handler.py
|
||||
IRPF90_temp
|
||||
IRPF90_man
|
||||
irpf90_entities
|
||||
tags
|
||||
irpf90.make
|
||||
Makefile
|
||||
Makefile.depend
|
||||
.ninja_log
|
||||
# Automatically created by $QP_ROOT/scripts/module/module_handler.py
|
||||
.ninja_deps
|
||||
ezfio_interface.irp.f
|
||||
Ezfio_files
|
||||
MO_Basis
|
||||
Utils
|
||||
.ninja_log
|
||||
AO_Basis
|
||||
Electrons
|
||||
Ezfio_files
|
||||
IRPF90_man
|
||||
IRPF90_temp
|
||||
MO_Basis
|
||||
Makefile
|
||||
Makefile.depend
|
||||
Nuclei
|
||||
Utils
|
||||
ezfio_interface.irp.f
|
||||
irpf90.make
|
||||
irpf90_entities
|
||||
print_mo
|
||||
tags
|
@ -90,32 +90,32 @@ Documentation
|
||||
routine.
|
||||
|
||||
|
||||
`perturb_buffer_by_mono_dipole_moment_z <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L686>`_
|
||||
`perturb_buffer_by_mono_dipole_moment_z <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L896>`_
|
||||
Applly pertubration ``dipole_moment_z`` to the buffer of determinants generated in the H_apply
|
||||
routine.
|
||||
|
||||
|
||||
`perturb_buffer_by_mono_epstein_nesbet <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L476>`_
|
||||
`perturb_buffer_by_mono_epstein_nesbet <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L161>`_
|
||||
Applly pertubration ``epstein_nesbet`` to the buffer of determinants generated in the H_apply
|
||||
routine.
|
||||
|
||||
|
||||
`perturb_buffer_by_mono_epstein_nesbet_2x2 <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L581>`_
|
||||
`perturb_buffer_by_mono_epstein_nesbet_2x2 <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L266>`_
|
||||
Applly pertubration ``epstein_nesbet_2x2`` to the buffer of determinants generated in the H_apply
|
||||
routine.
|
||||
|
||||
|
||||
`perturb_buffer_by_mono_epstein_nesbet_sc2 <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L371>`_
|
||||
`perturb_buffer_by_mono_epstein_nesbet_sc2 <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L581>`_
|
||||
Applly pertubration ``epstein_nesbet_sc2`` to the buffer of determinants generated in the H_apply
|
||||
routine.
|
||||
|
||||
|
||||
`perturb_buffer_by_mono_epstein_nesbet_sc2_no_projected <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L266>`_
|
||||
`perturb_buffer_by_mono_epstein_nesbet_sc2_no_projected <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L476>`_
|
||||
Applly pertubration ``epstein_nesbet_sc2_no_projected`` to the buffer of determinants generated in the H_apply
|
||||
routine.
|
||||
|
||||
|
||||
`perturb_buffer_by_mono_epstein_nesbet_sc2_projected <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L161>`_
|
||||
`perturb_buffer_by_mono_epstein_nesbet_sc2_projected <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L371>`_
|
||||
Applly pertubration ``epstein_nesbet_sc2_projected`` to the buffer of determinants generated in the H_apply
|
||||
routine.
|
||||
|
||||
@ -125,7 +125,7 @@ Documentation
|
||||
routine.
|
||||
|
||||
|
||||
`perturb_buffer_by_mono_moller_plesset <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L896>`_
|
||||
`perturb_buffer_by_mono_moller_plesset <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L686>`_
|
||||
Applly pertubration ``moller_plesset`` to the buffer of determinants generated in the H_apply
|
||||
routine.
|
||||
|
||||
@ -135,32 +135,32 @@ Documentation
|
||||
routine.
|
||||
|
||||
|
||||
`perturb_buffer_dipole_moment_z <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L635>`_
|
||||
`perturb_buffer_dipole_moment_z <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L845>`_
|
||||
Applly pertubration ``dipole_moment_z`` to the buffer of determinants generated in the H_apply
|
||||
routine.
|
||||
|
||||
|
||||
`perturb_buffer_epstein_nesbet <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L425>`_
|
||||
`perturb_buffer_epstein_nesbet <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L110>`_
|
||||
Applly pertubration ``epstein_nesbet`` to the buffer of determinants generated in the H_apply
|
||||
routine.
|
||||
|
||||
|
||||
`perturb_buffer_epstein_nesbet_2x2 <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L530>`_
|
||||
`perturb_buffer_epstein_nesbet_2x2 <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L215>`_
|
||||
Applly pertubration ``epstein_nesbet_2x2`` to the buffer of determinants generated in the H_apply
|
||||
routine.
|
||||
|
||||
|
||||
`perturb_buffer_epstein_nesbet_sc2 <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L320>`_
|
||||
`perturb_buffer_epstein_nesbet_sc2 <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L530>`_
|
||||
Applly pertubration ``epstein_nesbet_sc2`` to the buffer of determinants generated in the H_apply
|
||||
routine.
|
||||
|
||||
|
||||
`perturb_buffer_epstein_nesbet_sc2_no_projected <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L215>`_
|
||||
`perturb_buffer_epstein_nesbet_sc2_no_projected <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L425>`_
|
||||
Applly pertubration ``epstein_nesbet_sc2_no_projected`` to the buffer of determinants generated in the H_apply
|
||||
routine.
|
||||
|
||||
|
||||
`perturb_buffer_epstein_nesbet_sc2_projected <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L110>`_
|
||||
`perturb_buffer_epstein_nesbet_sc2_projected <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L320>`_
|
||||
Applly pertubration ``epstein_nesbet_sc2_projected`` to the buffer of determinants generated in the H_apply
|
||||
routine.
|
||||
|
||||
@ -170,7 +170,7 @@ Documentation
|
||||
routine.
|
||||
|
||||
|
||||
`perturb_buffer_moller_plesset <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L845>`_
|
||||
`perturb_buffer_moller_plesset <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/perturbation.irp.f_shell_13#L635>`_
|
||||
Applly pertubration ``moller_plesset`` to the buffer of determinants generated in the H_apply
|
||||
routine.
|
||||
|
||||
|
@ -1,36 +0,0 @@
|
||||
use bitmasks
|
||||
|
||||
BEGIN_PROVIDER [ integer(bit_kind), psi_ref, (N_int,2,psi_det_size) ]
|
||||
&BEGIN_PROVIDER [ double precision, psi_ref_coef, (psi_det_size,n_states) ]
|
||||
&BEGIN_PROVIDER [ integer, idx_ref, (psi_det_size) ]
|
||||
&BEGIN_PROVIDER [ integer, N_det_ref ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Reference wave function, defined as determinants with coefficients > 0.05
|
||||
! idx_ref gives the indice of the ref determinant in psi_det.
|
||||
END_DOC
|
||||
integer :: i, k, l
|
||||
logical :: good
|
||||
N_det_ref = 0
|
||||
do i=1,N_det
|
||||
good = .False.
|
||||
do l = 1, N_states
|
||||
psi_ref_coef(i,l) = 0.d0
|
||||
good = good.or.(dabs(psi_coef(i,l)) > 0.05d0)
|
||||
enddo
|
||||
if (good) then
|
||||
N_det_ref = N_det_ref+1
|
||||
do k=1,N_int
|
||||
psi_ref(k,1,N_det_ref) = psi_det(k,1,i)
|
||||
psi_ref(k,2,N_det_ref) = psi_det(k,2,i)
|
||||
enddo
|
||||
idx_ref(N_det_ref) = i
|
||||
do k=1,N_states
|
||||
psi_ref_coef(N_det_ref,k) = psi_coef(i,k)
|
||||
enddo
|
||||
endif
|
||||
enddo
|
||||
call write_int(output_determinants,N_det_ref, 'Number of determinants in the reference')
|
||||
|
||||
END_PROVIDER
|
||||
|
45
plugins/Psiref_Utils/psi_ref_excitations_operators.irp.f
Normal file
@ -0,0 +1,45 @@
|
||||
use bitmasks
|
||||
|
||||
BEGIN_PROVIDER [integer(bit_kind), holes_operators, (N_int,2)]
|
||||
&BEGIN_PROVIDER [integer(bit_kind), particles_operators, (N_int,2)]
|
||||
|
||||
BEGIN_DOC
|
||||
! holes_operators represents an array of integers where all the holes have
|
||||
! been done going from psi_ref to psi_non_ref
|
||||
! particles_operators represents an array of integers where all the particles have
|
||||
! been done going from psi_ref to psi_non_ref
|
||||
END_DOC
|
||||
holes_operators = 0_bit_kind
|
||||
particles_operators = 0_bit_kind
|
||||
implicit none
|
||||
integer(bit_kind), allocatable :: key_test(:,:)
|
||||
integer(bit_kind), allocatable :: holes(:,:),particles(:,:)
|
||||
allocate(key_test(N_int,2))
|
||||
allocate(holes(N_int,2),particles(N_int,2))
|
||||
integer :: i,j,k
|
||||
print*,'providing holes_operators and particles_operators'
|
||||
do i = 1, N_det_ref
|
||||
do j = 1, N_det_non_ref
|
||||
do k = 1, N_int
|
||||
key_test(k,1) = xor(psi_ref(k,1,i),psi_non_ref(k,1,j))
|
||||
key_test(k,2) = xor(psi_ref(k,2,i),psi_non_ref(k,2,j))
|
||||
enddo
|
||||
do k = 1,N_int
|
||||
holes(k,1) = iand(psi_ref(k,1,i),key_test(k,1))
|
||||
holes(k,2) = iand(psi_ref(k,2,i),key_test(k,2))
|
||||
particles(k,1) = iand(psi_non_ref(k,1,j),key_test(k,1))
|
||||
particles(k,2) = iand(psi_non_ref(k,2,j),key_test(k,2))
|
||||
enddo
|
||||
do k = 1, N_int
|
||||
holes_operators(k,1) = ior(holes_operators(k,1),holes(k,1))
|
||||
holes_operators(k,2) = ior(holes_operators(k,2),holes(k,2))
|
||||
particles_operators(k,1) = ior(particles_operators(k,1),particles(k,1))
|
||||
particles_operators(k,2) = ior(particles_operators(k,2),particles(k,2))
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
|
||||
deallocate(key_test)
|
||||
deallocate(holes,particles)
|
||||
|
||||
END_PROVIDER
|
@ -28,6 +28,7 @@ filterhole
|
||||
filterparticle
|
||||
do_double_excitations
|
||||
check_double_excitation
|
||||
filter_vvvv_excitation
|
||||
""".split()
|
||||
|
||||
class H_apply(object):
|
||||
@ -51,7 +52,7 @@ class H_apply(object):
|
||||
!$OMP accu,i_a,hole_tmp,particle_tmp,occ_particle_tmp, &
|
||||
!$OMP occ_hole_tmp,key_idx,i_b,j_b,key,N_elec_in_key_part_1,&
|
||||
!$OMP N_elec_in_key_hole_1,N_elec_in_key_part_2, &
|
||||
!$OMP N_elec_in_key_hole_2,ia_ja_pairs) &
|
||||
!$OMP N_elec_in_key_hole_2,ia_ja_pairs,key_union_hole_part) &
|
||||
!$OMP SHARED(key_in,N_int,elec_num_tab,mo_tot_num, &
|
||||
!$OMP hole_1, particl_1, hole_2, particl_2, &
|
||||
!$OMP elec_alpha_num,i_generator) FIRSTPRIVATE(iproc)"""
|
||||
@ -126,6 +127,21 @@ class H_apply(object):
|
||||
self["check_double_excitation"] = """
|
||||
check_double_excitation = .False.
|
||||
"""
|
||||
|
||||
def filter_vvvv_excitation(self):
|
||||
self["filter_vvvv_excitation"] = """
|
||||
key_union_hole_part = 0_bit_kind
|
||||
call set_bite_to_integer(i_a,key_union_hole_part,N_int)
|
||||
call set_bite_to_integer(j_a,key_union_hole_part,N_int)
|
||||
call set_bite_to_integer(i_b,key_union_hole_part,N_int)
|
||||
call set_bite_to_integer(j_b,key_union_hole_part,N_int)
|
||||
do jtest_vvvv = 1, N_int
|
||||
if(iand(key_union_hole_part(jtest_vvvv),virt_bitmask(jtest_vvvv,1).ne.key_union_hole_part(jtest_vvvv)))then
|
||||
b_cycle = .False.
|
||||
endif
|
||||
enddo
|
||||
if(b_cycle) cycle
|
||||
"""
|
||||
def set_filter_holes(self):
|
||||
self["filterhole"] = """
|
||||
if(iand(ibset(0_bit_kind,j),hole(k,other_spin)).eq.0_bit_kind )cycle
|
||||
|
@ -62,7 +62,7 @@ Documentation
|
||||
Transform a bit string to a string for printing
|
||||
|
||||
|
||||
`cas_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L173>`_
|
||||
`cas_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L220>`_
|
||||
Bitmasks for CAS reference determinants. (N_int, alpha/beta, CAS reference)
|
||||
|
||||
|
||||
@ -70,6 +70,10 @@ Documentation
|
||||
Bitmask to include all possible single excitations from Hartree-Fock
|
||||
|
||||
|
||||
`core_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L347>`_
|
||||
Reunion of the inactive, active and virtual bitmasks
|
||||
|
||||
|
||||
`debug_det <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks_routines.irp.f#L120>`_
|
||||
Subroutine to print the content of a determinant in '+-' notation and
|
||||
hexadecimal representation.
|
||||
@ -84,7 +88,27 @@ Documentation
|
||||
Bitmask to include all possible MOs
|
||||
|
||||
|
||||
`generators_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L100>`_
|
||||
`generators_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L147>`_
|
||||
Bitmasks for generator determinants.
|
||||
(N_int, alpha/beta, hole/particle, generator).
|
||||
.br
|
||||
3rd index is :
|
||||
.br
|
||||
* 1 : hole for single exc
|
||||
.br
|
||||
* 2 : particle for single exc
|
||||
.br
|
||||
* 3 : hole for 1st exc of double
|
||||
.br
|
||||
* 4 : particle for 1st exc of double
|
||||
.br
|
||||
* 5 : hole for 2nd exc of double
|
||||
.br
|
||||
* 6 : particle for 2nd exc of double
|
||||
.br
|
||||
|
||||
|
||||
`generators_bitmask_restart <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L103>`_
|
||||
Bitmasks for generator determinants.
|
||||
(N_int, alpha/beta, hole/particle, generator).
|
||||
.br
|
||||
@ -108,24 +132,36 @@ Documentation
|
||||
Hartree Fock bit mask
|
||||
|
||||
|
||||
`i_bitmask_gen <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L211>`_
|
||||
`i_bitmask_gen <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L361>`_
|
||||
Current bitmask for the generators
|
||||
|
||||
|
||||
`inact_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L193>`_
|
||||
`inact_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L251>`_
|
||||
Bitmasks for the inactive orbitals that are excited in post CAS method
|
||||
|
||||
|
||||
`inact_virt_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L335>`_
|
||||
Reunion of the inactive and virtual bitmasks
|
||||
|
||||
|
||||
`is_a_two_holes_two_particles <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmask_cas_routines.irp.f#L206>`_
|
||||
Undocumented
|
||||
|
||||
|
||||
`list_inact <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L301>`_
|
||||
Undocumented
|
||||
|
||||
|
||||
`list_to_bitstring <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks_routines.irp.f#L29>`_
|
||||
Returns the physical string "string(N_int,2)" from the array of
|
||||
occupations "list(N_int*bit_kind_size,2)
|
||||
|
||||
|
||||
`n_cas_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L143>`_
|
||||
`list_virt <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L302>`_
|
||||
Undocumented
|
||||
|
||||
|
||||
`n_cas_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L190>`_
|
||||
Number of bitmasks for CAS
|
||||
|
||||
|
||||
@ -133,10 +169,18 @@ Documentation
|
||||
Number of bitmasks for generators
|
||||
|
||||
|
||||
`n_inact_orb <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L253>`_
|
||||
Bitmasks for the inactive orbitals that are excited in post CAS method
|
||||
|
||||
|
||||
`n_int <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L3>`_
|
||||
Number of 64-bit integers needed to represent determinants as binary strings
|
||||
|
||||
|
||||
`n_virt_orb <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L254>`_
|
||||
Bitmasks for the inactive orbitals that are excited in post CAS method
|
||||
|
||||
|
||||
`number_of_holes <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmask_cas_routines.irp.f#L1>`_
|
||||
Undocumented
|
||||
|
||||
@ -165,6 +209,14 @@ Documentation
|
||||
Reference bit mask, used in Slater rules, chosen as Hartree-Fock bitmask
|
||||
|
||||
|
||||
`virt_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L194>`_
|
||||
`reunion_of_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L322>`_
|
||||
Reunion of the inactive, active and virtual bitmasks
|
||||
|
||||
|
||||
`unpaired_alpha_electrons <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L370>`_
|
||||
Bitmask reprenting the unpaired alpha electrons in the HF_bitmask
|
||||
|
||||
|
||||
`virt_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L252>`_
|
||||
Bitmasks for the inactive orbitals that are excited in post CAS method
|
||||
|
||||
|
@ -97,6 +97,53 @@ BEGIN_PROVIDER [ integer, N_generators_bitmask ]
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
|
||||
|
||||
|
||||
BEGIN_PROVIDER [ integer(bit_kind), generators_bitmask_restart, (N_int,2,6,N_generators_bitmask) ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Bitmasks for generator determinants.
|
||||
! (N_int, alpha/beta, hole/particle, generator).
|
||||
!
|
||||
! 3rd index is :
|
||||
!
|
||||
! * 1 : hole for single exc
|
||||
!
|
||||
! * 2 : particle for single exc
|
||||
!
|
||||
! * 3 : hole for 1st exc of double
|
||||
!
|
||||
! * 4 : particle for 1st exc of double
|
||||
!
|
||||
! * 5 : hole for 2nd exc of double
|
||||
!
|
||||
! * 6 : particle for 2nd exc of double
|
||||
!
|
||||
END_DOC
|
||||
logical :: exists
|
||||
PROVIDE ezfio_filename
|
||||
|
||||
call ezfio_has_bitmasks_generators(exists)
|
||||
if (exists) then
|
||||
call ezfio_get_bitmasks_generators(generators_bitmask_restart)
|
||||
else
|
||||
integer :: k, ispin
|
||||
do k=1,N_generators_bitmask
|
||||
do ispin=1,2
|
||||
generators_bitmask_restart(:,ispin,s_hole ,k) = full_ijkl_bitmask(:,d_hole1)
|
||||
generators_bitmask_restart(:,ispin,s_part ,k) = full_ijkl_bitmask(:,d_part1)
|
||||
generators_bitmask_restart(:,ispin,d_hole1,k) = full_ijkl_bitmask(:,d_hole1)
|
||||
generators_bitmask_restart(:,ispin,d_part1,k) = full_ijkl_bitmask(:,d_part1)
|
||||
generators_bitmask_restart(:,ispin,d_hole2,k) = full_ijkl_bitmask(:,d_hole2)
|
||||
generators_bitmask_restart(:,ispin,d_part2,k) = full_ijkl_bitmask(:,d_part2)
|
||||
enddo
|
||||
enddo
|
||||
endif
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
|
||||
BEGIN_PROVIDER [ integer(bit_kind), generators_bitmask, (N_int,2,6,N_generators_bitmask) ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
@ -176,38 +223,144 @@ BEGIN_PROVIDER [ integer(bit_kind), cas_bitmask, (N_int,2,N_cas_bitmask) ]
|
||||
! Bitmasks for CAS reference determinants. (N_int, alpha/beta, CAS reference)
|
||||
END_DOC
|
||||
logical :: exists
|
||||
integer :: i
|
||||
integer :: i,i_part,i_gen,j
|
||||
PROVIDE ezfio_filename
|
||||
|
||||
call ezfio_has_bitmasks_cas(exists)
|
||||
if (exists) then
|
||||
print*,'---------------------'
|
||||
print*,'CAS BITMASK RESTART'
|
||||
call ezfio_get_bitmasks_cas(cas_bitmask)
|
||||
print*,'---------------------'
|
||||
else
|
||||
if(N_generators_bitmask == 1)then
|
||||
do i=1,N_cas_bitmask
|
||||
cas_bitmask(:,:,i) = iand(not(HF_bitmask(:,:)),full_ijkl_bitmask(:,:))
|
||||
enddo
|
||||
else
|
||||
i_part = 2
|
||||
i_gen = 1
|
||||
do j = 1, N_cas_bitmask
|
||||
do i = 1, N_int
|
||||
cas_bitmask(i,1,j) = generators_bitmask_restart(i,1,i_part,i_gen)
|
||||
cas_bitmask(i,2,j) = generators_bitmask_restart(i,2,i_part,i_gen)
|
||||
enddo
|
||||
enddo
|
||||
endif
|
||||
endif
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
BEGIN_PROVIDER [ integer(bit_kind), inact_bitmask, (N_int,2) ]
|
||||
&BEGIN_PROVIDER [ integer(bit_kind), virt_bitmask, (N_int,2) ]
|
||||
&BEGIN_PROVIDER [ integer, n_inact_orb ]
|
||||
&BEGIN_PROVIDER [ integer, n_virt_orb ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Bitmasks for the inactive orbitals that are excited in post CAS method
|
||||
END_DOC
|
||||
logical :: exists
|
||||
integer :: j
|
||||
integer :: j,i
|
||||
integer :: i_hole,i_part,i_gen
|
||||
PROVIDE ezfio_filename
|
||||
do j = 1, N_int
|
||||
inact_bitmask(j,1) = xor(generators_bitmask(j,1,1,1),cas_bitmask(j,1,1))
|
||||
inact_bitmask(j,2) = xor(generators_bitmask(j,2,1,1),cas_bitmask(j,2,1))
|
||||
virt_bitmask(j,1) = xor(generators_bitmask(j,1,2,1),cas_bitmask(j,1,1))
|
||||
virt_bitmask(j,2) = xor(generators_bitmask(j,2,2,1),cas_bitmask(j,2,1))
|
||||
enddo
|
||||
!do j = 1, N_int
|
||||
! inact_bitmask(j,1) = xor(generators_bitmask(j,1,1,1),cas_bitmask(j,1,1))
|
||||
! inact_bitmask(j,2) = xor(generators_bitmask(j,2,1,1),cas_bitmask(j,2,1))
|
||||
! virt_bitmask(j,1) = xor(generators_bitmask(j,1,2,1),cas_bitmask(j,1,1))
|
||||
! virt_bitmask(j,2) = xor(generators_bitmask(j,2,2,1),cas_bitmask(j,2,1))
|
||||
!enddo
|
||||
n_inact_orb = 0
|
||||
n_virt_orb = 0
|
||||
if(N_generators_bitmask == 1)then
|
||||
do j = 1, N_int
|
||||
inact_bitmask(j,1) = xor(generators_bitmask_restart(j,1,1,1),cas_bitmask(j,1,1))
|
||||
inact_bitmask(j,2) = xor(generators_bitmask_restart(j,2,1,1),cas_bitmask(j,2,1))
|
||||
virt_bitmask(j,1) = xor(generators_bitmask_restart(j,1,2,1),cas_bitmask(j,1,1))
|
||||
virt_bitmask(j,2) = xor(generators_bitmask_restart(j,2,2,1),cas_bitmask(j,2,1))
|
||||
n_inact_orb += popcnt(inact_bitmask(j,1))
|
||||
n_virt_orb += popcnt(virt_bitmask(j,1))
|
||||
enddo
|
||||
else
|
||||
i_hole = 1
|
||||
i_gen = 1
|
||||
do i = 1, N_int
|
||||
inact_bitmask(i,1) = generators_bitmask(i,1,i_hole,i_gen)
|
||||
inact_bitmask(i,2) = generators_bitmask(i,2,i_hole,i_gen)
|
||||
n_inact_orb += popcnt(inact_bitmask(i,1))
|
||||
enddo
|
||||
i_part = 2
|
||||
i_gen = 3
|
||||
do i = 1, N_int
|
||||
virt_bitmask(i,1) = generators_bitmask(i,1,i_part,i_gen)
|
||||
virt_bitmask(i,2) = generators_bitmask(i,2,i_part,i_gen)
|
||||
n_virt_orb += popcnt(virt_bitmask(i,1))
|
||||
enddo
|
||||
endif
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
|
||||
|
||||
BEGIN_PROVIDER [ integer, list_inact, (n_inact_orb)]
|
||||
&BEGIN_PROVIDER [ integer, list_virt, (n_virt_orb)]
|
||||
implicit none
|
||||
integer :: occ_inact(N_int*bit_kind_size)
|
||||
integer :: itest,i
|
||||
occ_inact = 0
|
||||
call bitstring_to_list(inact_bitmask(1,1), occ_inact(1), itest, N_int)
|
||||
ASSERT(itest==n_inact_orb)
|
||||
do i = 1, n_inact_orb
|
||||
list_inact(i) = occ_inact(i)
|
||||
enddo
|
||||
|
||||
occ_inact = 0
|
||||
call bitstring_to_list(virt_bitmask(1,1), occ_inact(1), itest, N_int)
|
||||
ASSERT(itest==n_virt_orb)
|
||||
do i = 1, n_virt_orb
|
||||
list_virt(i) = occ_inact(i)
|
||||
enddo
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
BEGIN_PROVIDER [ integer(bit_kind), reunion_of_bitmask, (N_int,2)]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Reunion of the inactive, active and virtual bitmasks
|
||||
END_DOC
|
||||
integer :: i,j
|
||||
do i = 1, N_int
|
||||
reunion_of_bitmask(i,1) = ior(ior(cas_bitmask(i,1,1),inact_bitmask(i,1)),virt_bitmask(i,1))
|
||||
reunion_of_bitmask(i,2) = ior(ior(cas_bitmask(i,2,1),inact_bitmask(i,2)),virt_bitmask(i,2))
|
||||
enddo
|
||||
END_PROVIDER
|
||||
|
||||
|
||||
BEGIN_PROVIDER [ integer(bit_kind), inact_virt_bitmask, (N_int,2)]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Reunion of the inactive and virtual bitmasks
|
||||
END_DOC
|
||||
integer :: i,j
|
||||
do i = 1, N_int
|
||||
inact_virt_bitmask(i,1) = ior(inact_bitmask(i,1),virt_bitmask(i,1))
|
||||
inact_virt_bitmask(i,2) = ior(inact_bitmask(i,2),virt_bitmask(i,2))
|
||||
enddo
|
||||
END_PROVIDER
|
||||
|
||||
BEGIN_PROVIDER [ integer(bit_kind), core_bitmask, (N_int,2)]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Reunion of the inactive, active and virtual bitmasks
|
||||
END_DOC
|
||||
integer :: i,j
|
||||
do i = 1, N_int
|
||||
core_bitmask(i,1) = iand(ref_bitmask(i,1),reunion_of_bitmask(i,1))
|
||||
core_bitmask(i,2) = iand(ref_bitmask(i,2),reunion_of_bitmask(i,2))
|
||||
enddo
|
||||
END_PROVIDER
|
||||
|
||||
|
||||
|
||||
BEGIN_PROVIDER [ integer, i_bitmask_gen ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
@ -217,3 +370,14 @@ BEGIN_PROVIDER [ integer, i_bitmask_gen ]
|
||||
END_PROVIDER
|
||||
|
||||
|
||||
BEGIN_PROVIDER [ integer(bit_kind), unpaired_alpha_electrons, (N_int)]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Bitmask reprenting the unpaired alpha electrons in the HF_bitmask
|
||||
END_DOC
|
||||
integer :: i
|
||||
unpaired_alpha_electrons = 0_bit_kind
|
||||
do i = 1, N_int
|
||||
unpaired_alpha_electrons(i) = xor(HF_bitmask(i,1),HF_bitmask(i,2))
|
||||
enddo
|
||||
END_PROVIDER
|
||||
|
4
src/Determinants/.gitignore
vendored
@ -16,13 +16,17 @@ Nuclei
|
||||
Pseudo
|
||||
Utils
|
||||
det_svd
|
||||
diag_and_save
|
||||
ezfio_interface.irp.f
|
||||
guess_doublet
|
||||
guess_singlet
|
||||
guess_triplet
|
||||
irpf90.make
|
||||
irpf90_entities
|
||||
print_cas_energy
|
||||
print_s2
|
||||
program_initial_determinants
|
||||
save_natorb
|
||||
save_wf_only_monos
|
||||
tags
|
||||
truncate_wf
|
@ -18,6 +18,7 @@ subroutine $subroutine_diexc(key_in, hole_1,particl_1, hole_2, particl_2, i_gene
|
||||
integer(bit_kind), allocatable :: hole_save(:,:)
|
||||
integer(bit_kind), allocatable :: key(:,:),hole(:,:), particle(:,:)
|
||||
integer(bit_kind), allocatable :: hole_tmp(:,:), particle_tmp(:,:)
|
||||
integer(bit_kind), allocatable :: key_union_hole_part(:)
|
||||
integer :: ii,i,jj,j,k,ispin,l
|
||||
integer, allocatable :: occ_particle(:,:), occ_hole(:,:)
|
||||
integer, allocatable :: occ_particle_tmp(:,:), occ_hole_tmp(:,:)
|
||||
@ -31,6 +32,7 @@ subroutine $subroutine_diexc(key_in, hole_1,particl_1, hole_2, particl_2, i_gene
|
||||
integer, allocatable :: ib_jb_pairs(:,:)
|
||||
double precision :: diag_H_mat_elem
|
||||
integer :: iproc
|
||||
integer :: jtest_vvvv
|
||||
integer(omp_lock_kind), save :: lck, ifirst=0
|
||||
if (ifirst == 0) then
|
||||
!$ call omp_init_lock(lck)
|
||||
@ -38,6 +40,7 @@ subroutine $subroutine_diexc(key_in, hole_1,particl_1, hole_2, particl_2, i_gene
|
||||
endif
|
||||
|
||||
logical :: check_double_excitation
|
||||
logical :: b_cycle
|
||||
check_double_excitation = .True.
|
||||
iproc = iproc_in
|
||||
|
||||
@ -50,7 +53,7 @@ subroutine $subroutine_diexc(key_in, hole_1,particl_1, hole_2, particl_2, i_gene
|
||||
key(N_int,2),hole(N_int,2), particle(N_int,2), hole_tmp(N_int,2),&
|
||||
particle_tmp(N_int,2), occ_particle(N_int*bit_kind_size,2), &
|
||||
occ_hole(N_int*bit_kind_size,2), occ_particle_tmp(N_int*bit_kind_size,2),&
|
||||
occ_hole_tmp(N_int*bit_kind_size,2))
|
||||
occ_hole_tmp(N_int*bit_kind_size,2),key_union_hole_part(N_int))
|
||||
$init_thread
|
||||
|
||||
|
||||
@ -151,6 +154,7 @@ subroutine $subroutine_diexc(key_in, hole_1,particl_1, hole_2, particl_2, i_gene
|
||||
ASSERT (j_b > 0)
|
||||
ASSERT (j_b <= mo_tot_num)
|
||||
if (array_pairs(i_b,j_b)) then
|
||||
$filter_vvvv_excitation
|
||||
i+= 1
|
||||
ib_jb_pairs(1,i) = i_b
|
||||
ib_jb_pairs(2,i) = j_b
|
||||
@ -200,6 +204,7 @@ subroutine $subroutine_diexc(key_in, hole_1,particl_1, hole_2, particl_2, i_gene
|
||||
ASSERT (j_b <= mo_tot_num)
|
||||
if (j_b <= j_a) cycle
|
||||
if (array_pairs(i_b,j_b)) then
|
||||
$filter_vvvv_excitation
|
||||
i+= 1
|
||||
ib_jb_pairs(1,i) = i_b
|
||||
ib_jb_pairs(2,i) = j_b
|
||||
@ -245,7 +250,7 @@ subroutine $subroutine_diexc(key_in, hole_1,particl_1, hole_2, particl_2, i_gene
|
||||
key,hole, particle, hole_tmp,&
|
||||
particle_tmp, occ_particle, &
|
||||
occ_hole, occ_particle_tmp,&
|
||||
occ_hole_tmp,array_pairs)
|
||||
occ_hole_tmp,array_pairs,key_union_hole_part)
|
||||
$omp_end_parallel
|
||||
$finalization
|
||||
end
|
||||
@ -278,6 +283,7 @@ subroutine $subroutine_monoexc(key_in, hole_1,particl_1,i_generator,iproc_in $pa
|
||||
integer :: N_elec_in_key_hole_1(2),N_elec_in_key_part_1(2)
|
||||
integer :: N_elec_in_key_hole_2(2),N_elec_in_key_part_2(2)
|
||||
logical :: is_a_two_holes_two_particles
|
||||
integer(bit_kind), allocatable :: key_union_hole_part(:)
|
||||
|
||||
integer, allocatable :: ia_ja_pairs(:,:,:)
|
||||
logical, allocatable :: array_pairs(:,:)
|
||||
@ -305,7 +311,7 @@ subroutine $subroutine_monoexc(key_in, hole_1,particl_1,i_generator,iproc_in $pa
|
||||
key(N_int,2),hole(N_int,2), particle(N_int,2), hole_tmp(N_int,2),&
|
||||
particle_tmp(N_int,2), occ_particle(N_int*bit_kind_size,2), &
|
||||
occ_hole(N_int*bit_kind_size,2), occ_particle_tmp(N_int*bit_kind_size,2),&
|
||||
occ_hole_tmp(N_int*bit_kind_size,2))
|
||||
occ_hole_tmp(N_int*bit_kind_size,2),key_union_hole_part(N_int))
|
||||
$init_thread
|
||||
!!!! First couple hole particle
|
||||
do j = 1, N_int
|
||||
@ -376,7 +382,7 @@ subroutine $subroutine_monoexc(key_in, hole_1,particl_1,i_generator,iproc_in $pa
|
||||
key,hole, particle, hole_tmp,&
|
||||
particle_tmp, occ_particle, &
|
||||
occ_hole, occ_particle_tmp,&
|
||||
occ_hole_tmp)
|
||||
occ_hole_tmp,key_union_hole_part)
|
||||
$omp_end_parallel
|
||||
$finalization
|
||||
|
||||
|
@ -221,7 +221,7 @@ Documentation
|
||||
Build connection proxy between determinants
|
||||
|
||||
|
||||
`det_num <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ezfio_interface.irp.f#L248>`_
|
||||
`det_num <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ezfio_interface.irp.f#L116>`_
|
||||
det_num
|
||||
|
||||
|
||||
@ -621,6 +621,10 @@ Documentation
|
||||
Undocumented
|
||||
|
||||
|
||||
`print_psi_cas <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/print_cas_energy.irp.f#L1>`_
|
||||
Undocumented
|
||||
|
||||
|
||||
`psi_average_norm_contrib <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L273>`_
|
||||
Contribution of determinants to the state-averaged density
|
||||
|
||||
@ -831,7 +835,11 @@ Documentation
|
||||
Undocumented
|
||||
|
||||
|
||||
`s2_eig <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ezfio_interface.irp.f#L116>`_
|
||||
`routine_count_mono_save_mono <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/save_wf_only_monos.irp.f#L9>`_
|
||||
Undocumented
|
||||
|
||||
|
||||
`s2_eig <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ezfio_interface.irp.f#L248>`_
|
||||
Force the wave function to be an eigenfunction of S^2
|
||||
|
||||
|
||||
@ -863,10 +871,22 @@ Documentation
|
||||
Save the wave function into the EZFIO file
|
||||
|
||||
|
||||
`save_wavefunction_specified <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L752>`_
|
||||
Save the wave function into the EZFIO file
|
||||
|
||||
|
||||
`save_wavefunction_unsorted <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L655>`_
|
||||
Save the wave function into the EZFIO file
|
||||
|
||||
|
||||
`save_wf <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/save_wf_only_monos.irp.f#L1>`_
|
||||
Undocumented
|
||||
|
||||
|
||||
`set_bite_to_integer <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/create_excitations.irp.f#L38>`_
|
||||
Undocumented
|
||||
|
||||
|
||||
`set_natural_mos <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/density_matrix.irp.f#L180>`_
|
||||
Set natural orbitals, obtained by diagonalization of the one-body density matrix in the MO basis
|
||||
|
||||
|
@ -34,3 +34,14 @@ subroutine do_mono_excitation(key_in,i_hole,i_particle,ispin,i_ok)
|
||||
i_ok = -1
|
||||
endif
|
||||
end
|
||||
|
||||
subroutine set_bite_to_integer(i_physical,key,Nint)
|
||||
use bitmasks
|
||||
implicit none
|
||||
integer, intent(in) :: i_physical,Nint
|
||||
integer(bit_kind), intent(inout) :: key(Nint)
|
||||
integer :: k,j,i
|
||||
k = ishft(i_physical-1,-bit_kind_shift)+1
|
||||
j = i_physical-ishft(k-1,bit_kind_shift)-1
|
||||
key(k) = ibset(key(k),j)
|
||||
end
|
||||
|
@ -12,7 +12,7 @@ BEGIN_PROVIDER [ integer, davidson_sze_max ]
|
||||
! Max number of Davidson sizes
|
||||
END_DOC
|
||||
ASSERT (davidson_sze_max <= davidson_iter_max)
|
||||
davidson_sze_max = 8*N_states_diag
|
||||
davidson_sze_max = min(8,2*N_states_diag)
|
||||
END_PROVIDER
|
||||
|
||||
subroutine davidson_diag(dets_in,u_in,energies,dim_in,sze,N_st,Nint,iunit)
|
||||
|
@ -749,3 +749,91 @@ end
|
||||
|
||||
|
||||
|
||||
subroutine save_wavefunction_specified(ndet,nstates,psidet,psicoef,ndetsave,index_det_save)
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Save the wave function into the EZFIO file
|
||||
END_DOC
|
||||
use bitmasks
|
||||
integer, intent(in) :: ndet,nstates
|
||||
integer(bit_kind), intent(in) :: psidet(N_int,2,ndet)
|
||||
double precision, intent(in) :: psicoef(ndet,nstates)
|
||||
integer, intent(in) :: index_det_save(ndet)
|
||||
integer, intent(in) :: ndetsave
|
||||
integer*8, allocatable :: psi_det_save(:,:,:)
|
||||
double precision, allocatable :: psi_coef_save(:,:)
|
||||
integer*8 :: det_8(100)
|
||||
integer(bit_kind) :: det_bk((100*8)/bit_kind)
|
||||
integer :: N_int2
|
||||
equivalence (det_8, det_bk)
|
||||
|
||||
integer :: i,k
|
||||
|
||||
PROVIDE progress_bar
|
||||
call start_progress(7,'Saving wfunction',0.d0)
|
||||
|
||||
progress_bar(1) = 1
|
||||
progress_value = dble(progress_bar(1))
|
||||
call ezfio_set_determinants_N_int(N_int)
|
||||
progress_bar(1) = 2
|
||||
progress_value = dble(progress_bar(1))
|
||||
call ezfio_set_determinants_bit_kind(bit_kind)
|
||||
progress_bar(1) = 3
|
||||
progress_value = dble(progress_bar(1))
|
||||
call ezfio_set_determinants_N_det(ndetsave)
|
||||
progress_bar(1) = 4
|
||||
progress_value = dble(progress_bar(1))
|
||||
call ezfio_set_determinants_n_states(nstates)
|
||||
progress_bar(1) = 5
|
||||
progress_value = dble(progress_bar(1))
|
||||
call ezfio_set_determinants_mo_label(mo_label)
|
||||
|
||||
progress_bar(1) = 6
|
||||
progress_value = dble(progress_bar(1))
|
||||
|
||||
N_int2 = (N_int*bit_kind)/8
|
||||
allocate (psi_det_save(N_int2,2,ndetsave))
|
||||
do i=1,ndetsave
|
||||
do k=1,N_int
|
||||
det_bk(k) = psidet(k,1,index_det_save(i))
|
||||
enddo
|
||||
do k=1,N_int2
|
||||
psi_det_save(k,1,i) = det_8(k)
|
||||
enddo
|
||||
do k=1,N_int
|
||||
det_bk(k) = psidet(k,2,index_det_save(i))
|
||||
enddo
|
||||
do k=1,N_int2
|
||||
psi_det_save(k,2,i) = det_8(k)
|
||||
enddo
|
||||
enddo
|
||||
call ezfio_set_determinants_psi_det(psi_det_save)
|
||||
deallocate (psi_det_save)
|
||||
|
||||
progress_bar(1) = 7
|
||||
progress_value = dble(progress_bar(1))
|
||||
allocate (psi_coef_save(ndetsave,nstates))
|
||||
double precision :: accu_norm(nstates)
|
||||
accu_norm = 0.d0
|
||||
do k=1,nstates
|
||||
do i=1,ndetsave
|
||||
accu_norm(k) = accu_norm(k) + psicoef(index_det_save(i),k) * psicoef(index_det_save(i),k)
|
||||
psi_coef_save(i,k) = psicoef(index_det_save(i),k)
|
||||
enddo
|
||||
enddo
|
||||
do k = 1, nstates
|
||||
accu_norm(k) = 1.d0/dsqrt(accu_norm(k))
|
||||
enddo
|
||||
do k=1,nstates
|
||||
do i=1,ndetsave
|
||||
psi_coef_save(i,k) = psi_coef_save(i,k) * accu_norm(k)
|
||||
enddo
|
||||
enddo
|
||||
|
||||
call ezfio_set_determinants_psi_coef(psi_coef_save)
|
||||
call write_int(output_determinants,ndet,'Saved determinants')
|
||||
call stop_progress
|
||||
deallocate (psi_coef_save)
|
||||
end
|
||||
|
||||
|
||||
|
@ -1095,13 +1095,9 @@ subroutine H_u_0(v_0,u_0,H_jj,n,keys_tmp,Nint)
|
||||
!$OMP PARALLEL DEFAULT(NONE) &
|
||||
!$OMP PRIVATE(i,hij,j,k,idx,jj,vt) &
|
||||
!$OMP SHARED(n,H_jj,u_0,keys_tmp,Nint,v_0,davidson_threshold)
|
||||
!$OMP DO SCHEDULE(static)
|
||||
do i=1,n
|
||||
v_0(i) = H_jj(i) * u_0(i)
|
||||
enddo
|
||||
!$OMP END DO
|
||||
allocate(idx(0:n), vt(n))
|
||||
Vt = 0.d0
|
||||
v_0 = 0.d0
|
||||
!$OMP DO SCHEDULE(guided)
|
||||
do i=1,n
|
||||
idx(0) = i
|
||||
@ -1123,6 +1119,9 @@ subroutine H_u_0(v_0,u_0,H_jj,n,keys_tmp,Nint)
|
||||
!$OMP END CRITICAL
|
||||
deallocate(idx,vt)
|
||||
!$OMP END PARALLEL
|
||||
do i=1,n
|
||||
v_0(i) += H_jj(i) * u_0(i)
|
||||
enddo
|
||||
end
|
||||
|
||||
|
||||
|
164
src/Ezfio_files/README.rst
Normal file
@ -0,0 +1,164 @@
|
||||
==================
|
||||
Ezfio_files Module
|
||||
==================
|
||||
|
||||
This modules essentially contains the name of the EZFIO directory in the
|
||||
``ezfio_filename`` variable. This is read as the first argument of the
|
||||
command-line, or as the ``QP_INPUT`` environment variable.
|
||||
Documentation
|
||||
=============
|
||||
|
||||
.. Do not edit this section. It was auto-generated from the
|
||||
.. by the `update_README.py` script.
|
||||
|
||||
`ezfio_filename <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/ezfio.irp.f#L1>`_
|
||||
Name of EZFIO file. It is obtained from the QPACKAGE_INPUT environment
|
||||
variable if it is set, or as the 1st argument of the command line.
|
||||
|
||||
|
||||
`getunitandopen <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/get_unit_and_open.irp.f#L1>`_
|
||||
:f:
|
||||
file name
|
||||
.br
|
||||
:mode:
|
||||
'R' : READ, UNFORMATTED
|
||||
'W' : WRITE, UNFORMATTED
|
||||
'r' : READ, FORMATTED
|
||||
'w' : WRITE, FORMATTED
|
||||
'a' : APPEND, FORMATTED
|
||||
'x' : READ/WRITE, FORMATTED
|
||||
.br
|
||||
|
||||
|
||||
`output_ao_basis <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L1>`_
|
||||
Output file for AO_Basis
|
||||
|
||||
|
||||
`output_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L21>`_
|
||||
Output file for Bitmask
|
||||
|
||||
|
||||
`output_cas_sd <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L41>`_
|
||||
Output file for CAS_SD
|
||||
|
||||
|
||||
`output_cisd <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L61>`_
|
||||
Output file for CISD
|
||||
|
||||
|
||||
`output_cisd_sc2_selected <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L81>`_
|
||||
Output file for CISD_SC2_selected
|
||||
|
||||
|
||||
`output_cisd_selected <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L101>`_
|
||||
Output file for CISD_selected
|
||||
|
||||
|
||||
`output_cpu_time_0 <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f#L2>`_
|
||||
Initial CPU and wall times when printing in the output files
|
||||
|
||||
|
||||
`output_ddci_selected <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L121>`_
|
||||
Output file for DDCI_selected
|
||||
|
||||
|
||||
`output_determinants <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L141>`_
|
||||
Output file for Determinants
|
||||
|
||||
|
||||
`output_electrons <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L161>`_
|
||||
Output file for Electrons
|
||||
|
||||
|
||||
`output_ezfio_files <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L181>`_
|
||||
Output file for Ezfio_files
|
||||
|
||||
|
||||
`output_full_ci <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L201>`_
|
||||
Output file for Full_CI
|
||||
|
||||
|
||||
`output_generators_cas <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L221>`_
|
||||
Output file for Generators_CAS
|
||||
|
||||
|
||||
`output_generators_full <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L241>`_
|
||||
Output file for Generators_full
|
||||
|
||||
|
||||
`output_hartree_fock <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L261>`_
|
||||
Output file for Hartree_Fock
|
||||
|
||||
|
||||
`output_integrals_bielec <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L281>`_
|
||||
Output file for Integrals_Bielec
|
||||
|
||||
|
||||
`output_integrals_monoelec <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L301>`_
|
||||
Output file for Integrals_Monoelec
|
||||
|
||||
|
||||
`output_loc_cele <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L321>`_
|
||||
Output file for loc_cele
|
||||
|
||||
|
||||
`output_mo_basis <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L341>`_
|
||||
Output file for MO_Basis
|
||||
|
||||
|
||||
`output_moguess <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L361>`_
|
||||
Output file for MOGuess
|
||||
|
||||
|
||||
`output_molden <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L381>`_
|
||||
Output file for Molden
|
||||
|
||||
|
||||
`output_nuclei <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L401>`_
|
||||
Output file for Nuclei
|
||||
|
||||
|
||||
`output_perturbation <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L421>`_
|
||||
Output file for Perturbation
|
||||
|
||||
|
||||
`output_properties <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L441>`_
|
||||
Output file for Properties
|
||||
|
||||
|
||||
`output_pseudo <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L461>`_
|
||||
Output file for Pseudo
|
||||
|
||||
|
||||
`output_selectors_full <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L481>`_
|
||||
Output file for Selectors_full
|
||||
|
||||
|
||||
`output_singlerefmethod <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L501>`_
|
||||
Output file for SingleRefMethod
|
||||
|
||||
|
||||
`output_utils <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f_shell_40#L521>`_
|
||||
Output file for Utils
|
||||
|
||||
|
||||
`output_wall_time_0 <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f#L1>`_
|
||||
Initial CPU and wall times when printing in the output files
|
||||
|
||||
|
||||
`write_bool <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f#L88>`_
|
||||
Write an logical value in output
|
||||
|
||||
|
||||
`write_double <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f#L58>`_
|
||||
Write a double precision value in output
|
||||
|
||||
|
||||
`write_int <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f#L73>`_
|
||||
Write an integer value in output
|
||||
|
||||
|
||||
`write_time <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files/output.irp.f#L42>`_
|
||||
Write a time stamp in the output for chronological reconstruction
|
||||
|
||||
|
@ -27,7 +27,7 @@ Documentation
|
||||
Array of the name of element, sorted by nuclear charge (integer)
|
||||
|
||||
|
||||
`nucl_charge <http://github.com/LCPQ/quantum_package/tree/master/src/Nuclei/ezfio_interface.irp.f#L24>`_
|
||||
`nucl_charge <http://github.com/LCPQ/quantum_package/tree/master/src/Nuclei/ezfio_interface.irp.f#L28>`_
|
||||
Nuclear charges
|
||||
|
||||
|
||||
@ -69,11 +69,11 @@ Documentation
|
||||
nucl_dist_vec : Nucleus-nucleus distances vectors
|
||||
|
||||
|
||||
`nucl_label <http://github.com/LCPQ/quantum_package/tree/master/src/Nuclei/ezfio_interface.irp.f#L6>`_
|
||||
`nucl_label <http://github.com/LCPQ/quantum_package/tree/master/src/Nuclei/ezfio_interface.irp.f#L50>`_
|
||||
Nuclear labels
|
||||
|
||||
|
||||
`nucl_num <http://github.com/LCPQ/quantum_package/tree/master/src/Nuclei/ezfio_interface.irp.f#L46>`_
|
||||
`nucl_num <http://github.com/LCPQ/quantum_package/tree/master/src/Nuclei/ezfio_interface.irp.f#L6>`_
|
||||
Number of nuclei
|
||||
|
||||
|
||||
|
@ -26,7 +26,7 @@ Documentation
|
||||
test
|
||||
|
||||
|
||||
`pseudo_dz_kl <http://github.com/LCPQ/quantum_package/tree/master/src/Pseudo/ezfio_interface.irp.f#L94>`_
|
||||
`pseudo_dz_kl <http://github.com/LCPQ/quantum_package/tree/master/src/Pseudo/ezfio_interface.irp.f#L226>`_
|
||||
test
|
||||
|
||||
|
||||
@ -42,7 +42,7 @@ Documentation
|
||||
test
|
||||
|
||||
|
||||
`pseudo_kmax <http://github.com/LCPQ/quantum_package/tree/master/src/Pseudo/ezfio_interface.irp.f#L72>`_
|
||||
`pseudo_kmax <http://github.com/LCPQ/quantum_package/tree/master/src/Pseudo/ezfio_interface.irp.f#L94>`_
|
||||
test
|
||||
|
||||
|
||||
@ -50,7 +50,7 @@ Documentation
|
||||
test
|
||||
|
||||
|
||||
`pseudo_n_k <http://github.com/LCPQ/quantum_package/tree/master/src/Pseudo/ezfio_interface.irp.f#L226>`_
|
||||
`pseudo_n_k <http://github.com/LCPQ/quantum_package/tree/master/src/Pseudo/ezfio_interface.irp.f#L72>`_
|
||||
test
|
||||
|
||||
|
||||
|