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https://github.com/LCPQ/quantum_package
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Fixed density matrix
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b9bda8dc27
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@ -85,7 +85,7 @@ module Xyz = struct
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let of_string s =
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let flush state accu number =
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let n =
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if (number = "") then 0
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if (number = "") then 1
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else (Int.of_string number)
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in
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match state with
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@ -251,7 +251,8 @@ subroutine give_2h1p_contrib_sec_order(matrix_2h1p)
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call get_mono_excitation(det_tmp,det_tmp_bis,exc,phase,N_int)
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! ! < det_tmp | H | det_tmp_bis > = F_{aorb,borb}
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hab = fock_operator_local(aorb,borb,kspin) * phase
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if(isnan(hab))then
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! if(isnan(hab))then
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if(hab /= hab)then
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print*, '2'
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stop
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endif
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@ -27,8 +27,8 @@ END_PROVIDER
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double precision :: ck, cl, ckl
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double precision :: phase
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integer :: h1,h2,p1,p2,s1,s2, degree
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integer(bit_kind) :: tmp_det(N_int,2), tmp_det2(N_int,2)
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integer :: exc(0:2,2,2),n_occ(2)
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integer(bit_kind) :: tmp_det(N_int,2), tmp_det2(N_int)
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integer :: exc(0:2,2),n_occ(2)
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double precision, allocatable :: tmp_a(:,:,:), tmp_b(:,:,:)
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integer :: krow, kcol, lrow, lcol
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@ -43,7 +43,7 @@ END_PROVIDER
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!$OMP elec_beta_num,one_body_dm_mo_alpha,one_body_dm_mo_beta,N_det,mo_tot_num_align,&
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!$OMP mo_tot_num,psi_bilinear_matrix_rows,psi_bilinear_matrix_columns, &
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!$OMP psi_bilinear_matrix_transp_rows, psi_bilinear_matrix_transp_columns, &
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!$OMP psi_bilinear_matrix_transp_order, psi_det_alpha_unique, psi_det_beta_unique, &
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!$OMP psi_bilinear_matrix_order_reverse, psi_det_alpha_unique, psi_det_beta_unique, &
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!$OMP psi_bilinear_matrix_values, psi_bilinear_matrix_transp_values)
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allocate(tmp_a(mo_tot_num_align,mo_tot_num,N_states), tmp_b(mo_tot_num_align,mo_tot_num,N_states) )
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tmp_a = 0.d0
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@ -70,22 +70,18 @@ END_PROVIDER
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l = k+1
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lrow = psi_bilinear_matrix_rows(l)
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lcol = psi_bilinear_matrix_columns(l)
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! Fix beta determinant, loop over alphas
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do while ( lcol == kcol )
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tmp_det2(:,1) = psi_det_alpha_unique(:, lrow)
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tmp_det2(:,2) = psi_det_beta_unique (:, lcol)
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call get_excitation_degree(tmp_det,tmp_det2,degree,N_int)
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tmp_det2(:) = psi_det_alpha_unique(:, lrow)
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call get_excitation_degree_spin(tmp_det(1,1),tmp_det2,degree,N_int)
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if (degree == 1) then
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call get_mono_excitation(psi_det(1,1,k),psi_det(1,1,l),exc,phase,N_int)
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call decode_exc(exc,degree,h1,p1,h2,p2,s1,s2)
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exc = 0
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call get_mono_excitation_spin(tmp_det(1,1),tmp_det2,exc,phase,N_int)
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call decode_exc_spin(exc,h1,p1,h2,p2)
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do m=1,N_states
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ckl = psi_bilinear_matrix_values(k,m)*psi_bilinear_matrix_values(l,m) * phase
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if (s1==1) then
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tmp_a(h1,p1,m) += ckl
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tmp_a(p1,h1,m) += ckl
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else
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tmp_b(h1,p1,m) += ckl
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tmp_b(p1,h1,m) += ckl
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endif
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enddo
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endif
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l = l+1
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@ -94,25 +90,20 @@ END_PROVIDER
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lcol = psi_bilinear_matrix_columns(l)
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enddo
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l = psi_bilinear_matrix_transp_order(k)+1
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l = psi_bilinear_matrix_order_reverse(k)+1
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! Fix alpha determinant, loop over betas
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lrow = psi_bilinear_matrix_transp_rows(l)
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lcol = psi_bilinear_matrix_transp_columns(l)
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do while ( lrow == krow )
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tmp_det2(:,1) = psi_det_alpha_unique(:, lrow)
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tmp_det2(:,2) = psi_det_beta_unique (:, lcol)
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call get_excitation_degree(tmp_det,tmp_det2,degree,N_int)
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tmp_det2(:) = psi_det_beta_unique (:, lcol)
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call get_excitation_degree_spin(tmp_det(1,2),tmp_det2,degree,N_int)
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if (degree == 1) then
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call get_mono_excitation(psi_det(1,1,k),psi_det(1,1,l),exc,phase,N_int)
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call decode_exc(exc,degree,h1,p1,h2,p2,s1,s2)
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call get_mono_excitation_spin(tmp_det(1,2),tmp_det2,exc,phase,N_int)
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call decode_exc_spin(exc,h1,p1,h2,p2)
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do m=1,N_states
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ckl = psi_bilinear_matrix_values(k,m)*psi_bilinear_matrix_transp_values(l,m) * phase
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if (s1==1) then
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tmp_a(h1,p1,m) += ckl
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tmp_a(p1,h1,m) += ckl
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else
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tmp_b(h1,p1,m) += ckl
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tmp_b(p1,h1,m) += ckl
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endif
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enddo
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endif
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l = l+1
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@ -317,3 +308,74 @@ END_PROVIDER
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END_PROVIDER
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BEGIN_PROVIDER [ double precision, one_body_dm_mo_alpha_old, (mo_tot_num_align,mo_tot_num,N_states) ]
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&BEGIN_PROVIDER [ double precision, one_body_dm_mo_beta_old, (mo_tot_num_align,mo_tot_num,N_states) ]
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implicit none
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BEGIN_DOC
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! Alpha and beta one-body density matrix for each state
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END_DOC
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integer :: j,k,l,m
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integer :: occ(N_int*bit_kind_size,2)
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double precision :: ck, cl, ckl
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double precision :: phase
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integer :: h1,h2,p1,p2,s1,s2, degree
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integer :: exc(0:2,2,2),n_occ(2)
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double precision, allocatable :: tmp_a(:,:,:), tmp_b(:,:,:)
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one_body_dm_mo_alpha_old = 0.d0
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one_body_dm_mo_beta_old = 0.d0
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!$OMP PARALLEL DEFAULT(NONE) &
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!$OMP PRIVATE(j,k,l,m,occ,ck, cl, ckl,phase,h1,h2,p1,p2,s1,s2, degree,exc, &
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!$OMP tmp_a, tmp_b, n_occ)&
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!$OMP SHARED(psi_det,psi_coef,N_int,N_states,elec_alpha_num,&
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!$OMP elec_beta_num,one_body_dm_mo_alpha_old,one_body_dm_mo_beta_old,N_det,mo_tot_num_align,&
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!$OMP mo_tot_num)
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allocate(tmp_a(mo_tot_num_align,mo_tot_num,N_states), tmp_b(mo_tot_num_align,mo_tot_num,N_states) )
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tmp_a = 0.d0
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tmp_b = 0.d0
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!$OMP DO SCHEDULE(dynamic)
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do k=1,N_det
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call bitstring_to_list_ab(psi_det(1,1,k), occ, n_occ, N_int)
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do m=1,N_states
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ck = psi_coef(k,m)*psi_coef(k,m)
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do l=1,elec_alpha_num
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j = occ(l,1)
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tmp_a(j,j,m) += ck
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enddo
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do l=1,elec_beta_num
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j = occ(l,2)
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tmp_b(j,j,m) += ck
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enddo
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enddo
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do l=1,k-1
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call get_excitation_degree(psi_det(1,1,k),psi_det(1,1,l),degree,N_int)
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if (degree /= 1) then
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cycle
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endif
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call get_mono_excitation(psi_det(1,1,k),psi_det(1,1,l),exc,phase,N_int)
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call decode_exc(exc,degree,h1,p1,h2,p2,s1,s2)
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do m=1,N_states
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ckl = psi_coef(k,m) * psi_coef(l,m) * phase
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if (s1==1) then
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tmp_a(h1,p1,m) += ckl
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tmp_a(p1,h1,m) += ckl
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else
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tmp_b(h1,p1,m) += ckl
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tmp_b(p1,h1,m) += ckl
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endif
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enddo
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enddo
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enddo
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!$OMP END DO NOWAIT
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!$OMP CRITICAL
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one_body_dm_mo_alpha_old(:,:,:) = one_body_dm_mo_alpha_old(:,:,:) + tmp_a(:,:,:)
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!$OMP END CRITICAL
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!$OMP CRITICAL
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one_body_dm_mo_beta_old(:,:,:) = one_body_dm_mo_beta_old(:,:,:) + tmp_b(:,:,:)
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!$OMP END CRITICAL
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deallocate(tmp_a,tmp_b)
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!$OMP END PARALLEL
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END_PROVIDER
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