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quantum_package/plugins/Selectors_full/selectors.irp.f

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Fortran
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use bitmasks
BEGIN_PROVIDER [ integer, psi_selectors_size ]
implicit none
psi_selectors_size = psi_det_size
END_PROVIDER
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BEGIN_PROVIDER [ integer, N_det_selectors]
implicit none
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BEGIN_DOC
! For Single reference wave functions, the number of selectors is 1 : the
! Hartree-Fock determinant
END_DOC
integer :: i
double precision :: norm
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call write_time(output_determinants)
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norm = 0.d0
N_det_selectors = N_det
do i=1,N_det
norm = norm + psi_average_norm_contrib_sorted(i)
if (norm > threshold_selectors) then
N_det_selectors = i-1
exit
endif
enddo
N_det_selectors = max(N_det_selectors,1)
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call write_int(output_determinants,N_det_selectors,'Number of selectors')
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END_PROVIDER
BEGIN_PROVIDER [ integer(bit_kind), psi_selectors, (N_int,2,psi_selectors_size) ]
&BEGIN_PROVIDER [ double precision, psi_selectors_coef, (psi_selectors_size,N_states) ]
implicit none
BEGIN_DOC
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! Determinants on which we apply <i|H|psi> for perturbation.
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END_DOC
integer :: i,k
do i=1,N_det_selectors
do k=1,N_int
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psi_selectors(k,1,i) = psi_det_sorted(k,1,i)
psi_selectors(k,2,i) = psi_det_sorted(k,2,i)
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enddo
enddo
do k=1,N_states
do i=1,N_det_selectors
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psi_selectors_coef(i,k) = psi_coef_sorted(i,k)
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enddo
enddo
END_PROVIDER
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BEGIN_PROVIDER [ double precision, psi_selectors_diag_h_mat, (psi_selectors_size) ]
implicit none
BEGIN_DOC
! Diagonal elements of the H matrix for each selectors
END_DOC
integer :: i
double precision :: diag_H_mat_elem
do i = 1, N_det_selectors
psi_selectors_diag_h_mat(i) = diag_H_mat_elem(psi_selectors(1,1,i),N_int)
enddo
END_PROVIDER
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BEGIN_PROVIDER [ integer(bit_kind), psi_selectors_ab, (N_int,2,psi_selectors_size) ]
&BEGIN_PROVIDER [ double precision, psi_selectors_coef_ab, (psi_selectors_size,N_states) ]
&BEGIN_PROVIDER [ integer, psi_selectors_next_ab, (2,psi_selectors_size) ]
implicit none
BEGIN_DOC
! Determinants on which we apply <i|H|j>.
! They are sorted by the 3 highest electrons in the alpha part,
! then by the 3 highest electrons in the beta part to accelerate
! the research of connected determinants.
END_DOC
integer :: i,j,k
integer, allocatable :: iorder(:)
integer*8, allocatable :: bit_tmp(:)
integer*8, external :: det_search_key
allocate ( iorder(N_det_selectors), bit_tmp(N_det_selectors) )
! Sort alpha dets
! ---------------
integer(bit_kind) :: det_tmp(N_int)
do i=1,N_det_selectors
iorder(i) = i
call int_of_3_highest_electrons(psi_selectors(1,1,i),bit_tmp(i),N_int)
enddo
call i8sort(bit_tmp,iorder,N_det_selectors)
!DIR$ IVDEP
do i=1,N_det_selectors
do j=1,N_int
psi_selectors_ab(j,1,i) = psi_selectors(j,1,iorder(i))
psi_selectors_ab(j,2,i) = psi_selectors(j,2,iorder(i))
enddo
do k=1,N_states
psi_coef_sorted_ab(i,k) = psi_selectors_coef(iorder(i),k)
enddo
enddo
! Find next alpha
! ---------------
integer :: next
next = N_det_selectors+1
psi_selectors_next_ab(1,N_det_selectors) = next
do i=N_det_selectors-1,1,-1
if (bit_tmp(i) /= bit_tmp(i+1)) then
next = i+1
endif
psi_selectors_next_ab(1,i) = next
enddo
! Sort beta dets
! --------------
integer :: istart, iend
integer(bit_kind), allocatable :: psi_selectors_ab_temp (:,:)
allocate ( psi_selectors_ab_temp (N_int,N_det_selectors) )
do i=1,N_det_selectors
do j=1,N_int
psi_selectors_ab_temp(j,i) = psi_selectors_ab(j,2,i)
enddo
iorder(i) = i
call int_of_3_highest_electrons(psi_selectors_ab_temp(1,i),bit_tmp(i),N_int)
enddo
istart=1
do while ( istart<N_det_selectors )
iend = psi_selectors_next_ab(1,istart)
call i8sort(bit_tmp(istart),iorder(istart),iend-istart)
!DIR$ IVDEP
do i=istart,iend-1
do j=1,N_int
psi_selectors_ab(j,2,i) = psi_selectors_ab_temp(j,iorder(i))
enddo
do k=1,N_states
psi_coef_sorted_ab(i,k) = psi_coef(iorder(i),k)
enddo
enddo
next = iend
psi_selectors_next_ab(2,iend-1) = next
do i=iend-2,1,-1
if (bit_tmp(i) /= bit_tmp(i+1)) then
next = i+1
endif
psi_selectors_next_ab(2,i) = next
enddo
istart = iend
enddo
deallocate(iorder, bit_tmp, psi_selectors_ab_temp)
END_PROVIDER