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quantum_package/plugins/QMC/truncate_wf_spin.irp.f
2018-05-07 15:51:02 +02:00

117 lines
3.4 KiB
Fortran

program truncate
read_wf = .True.
SOFT_TOUCH read_wf
call run
end
subroutine run
use bitmasks
implicit none
integer :: i,j,k, kk, nab, m, l
double precision :: norm, E, hij, num, ci, cj
integer, allocatable :: iorder(:)
double precision , allocatable :: norm_sort(:)
double precision :: e_0(N_states)
PROVIDE mo_bielec_integrals_in_map H_apply_buffer_allocated
nab = n_det_alpha_unique+n_det_beta_unique
allocate ( norm_sort(0:nab), iorder(0:nab) )
integer(bit_kind), allocatable :: det_i(:,:), det_j(:,:)
double precision, allocatable :: u_t(:,:), v_t(:,:), s_t(:,:)
double precision, allocatable :: u_0(:,:), v_0(:,:)
allocate(u_t(N_states,N_det),v_t(N_states,N_det),s_t(N_states,N_det))
allocate(u_0(N_det,N_states),v_0(N_det,N_states))
norm_sort(0) = 0.d0
iorder(0) = 0
do i=1,n_det_alpha_unique
norm_sort(i) = det_alpha_norm(i)
iorder(i) = i
enddo
do i=1,n_det_beta_unique
norm_sort(i+n_det_alpha_unique) = det_beta_norm(i)
iorder(i+n_det_alpha_unique) = -i
enddo
call dsort(norm_sort(1),iorder(1),nab)
PROVIDE psi_bilinear_matrix_values psi_bilinear_matrix_rows psi_bilinear_matrix_columns
PROVIDE nuclear_repulsion
print *, ''
do j=0,nab
i = iorder(j)
if (i<0) then
!$OMP PARALLEL DO PRIVATE(k)
do k=1,n_det
if (psi_bilinear_matrix_columns(k) == -i) then
do l=1,N_states
psi_bilinear_matrix_values(k,l) = 0.d0
enddo
endif
enddo
!$OMP END PARALLEL DO
else
!$OMP PARALLEL DO PRIVATE(k)
do k=1,n_det
if (psi_bilinear_matrix_rows(k) == i) then
do l=1,N_states
psi_bilinear_matrix_values(k,l) = 0.d0
enddo
endif
enddo
!$OMP END PARALLEL DO
endif
if (ci_threshold <= norm_sort(j)) then
exit
endif
enddo
m = 0
do k=1,n_det
if (sum(psi_bilinear_matrix_values(k,1:N_states)) /= 0.d0) then
m = m+1
endif
enddo
do k=1,N_states
E = E_0(k) + nuclear_repulsion
enddo
print *, 'Number of determinants:', m
call wf_of_psi_bilinear_matrix(.True.)
call save_wavefunction
u_0(1:N_det,1:N_states) = psi_bilinear_matrix_values(1:N_det,1:N_states)
v_0(1:N_det,1:N_states) = 0.d0
u_t(1:N_states,1:N_det) = 0.d0
v_t(1:N_states,1:N_det) = 0.d0
s_t(1:N_states,1:N_det) = 0.d0
call dtranspose( &
u_0, &
size(u_0, 1), &
u_t, &
size(u_t, 1), &
N_det, N_states)
print *, 'Computing H|Psi> ...'
call H_S2_u_0_nstates_openmp_work(v_t,s_t,u_t,N_states,N_det,1,N_det,0,1)
print *, 'Done'
call dtranspose( &
v_t, &
size(v_t, 1), &
v_0, &
size(v_0, 1), &
N_states, N_det)
double precision, external :: u_dot_u, u_dot_v
do i=1,N_states
e_0(i) = u_dot_v(u_0(1,i),v_0(1,i),N_det)/u_dot_u(u_0(1,i),N_det)
print *, 'E(',i,') = ', e_0(i) + nuclear_repulsion
enddo
deallocate (iorder, norm_sort)
end