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Merge pull request #189 from QuantumPackage/cleaning_dft
frozen core unset
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commit
3d63d39df8
@ -7,12 +7,13 @@ setting all MOs as Active, except the n/2 first ones which are set as Core.
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If pseudo-potentials are used, all the MOs are set as Active.
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Usage:
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qp_set_frozen_core [-q|--query] [(-l|-s|--large|--small)] EZFIO_DIR
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qp_set_frozen_core [-q|--query] [(-l|-s|-u|--large|--small|--unset)] EZFIO_DIR
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Options:
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-q --query Prints in the standard output the number of frozen MOs
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-l --large Use a small core
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-s --small Use a large core
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-u --unset Unset frozen core
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Default numbers of frozen electrons:
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@ -88,7 +89,9 @@ def main(arguments):
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elif charge <= 54: n_frozen += 9
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elif charge <= 86: n_frozen += 18
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elif charge <= 118: n_frozen += 27
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elif arguments["--unset"]:
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n_frozen = 0
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else: # default
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for charge in ezfio.nuclei_nucl_charge:
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if charge <= 4: pass
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@ -779,6 +779,7 @@ subroutine binary_search_cfg(cfgInp,addcfg)
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end subroutine
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BEGIN_PROVIDER [ integer, psi_configuration_to_psi_det, (2,N_configuration) ]
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&BEGIN_PROVIDER [ integer, psi_configuration_n_det, (N_configuration) ]
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&BEGIN_PROVIDER [ integer, psi_configuration_to_psi_det_data, (N_det) ]
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implicit none
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@ -867,6 +868,29 @@ end subroutine
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enddo
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deallocate(dets, old_order)
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integer :: ndet_conf
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do i = 1, N_configuration
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ndet_conf = psi_configuration_to_psi_det(2,i) - psi_configuration_to_psi_det(1,i) + 1
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psi_configuration_n_det(i) = ndet_conf
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enddo
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END_PROVIDER
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BEGIN_PROVIDER [ integer, n_elec_alpha_for_psi_configuration, (N_configuration)]
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implicit none
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integer :: i,j,k,l
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integer(bit_kind) :: det_tmp(N_int,2),det_alpha(N_int)
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n_elec_alpha_for_psi_configuration = 0
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do i = 1, N_configuration
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j = psi_configuration_to_psi_det(2,i)
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det_tmp(:,:) = psi_det(:,:,j)
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k = 0
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do l = 1, N_int
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det_alpha(N_int) = iand(det_tmp(l,1),psi_configuration(l,1,i))
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k += popcnt(det_alpha(l))
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enddo
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n_elec_alpha_for_psi_configuration(i) = k
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enddo
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END_PROVIDER
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@ -1,5 +1,5 @@
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subroutine davidson_general_ext_rout(u_in,H_jj,Dress_jj,energies,sze,N_st,N_st_diag_in,converged,hcalc)
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subroutine davidson_general_ext_rout_diag_dressed(u_in,H_jj,Dress_jj,energies,sze,N_st,N_st_diag_in,converged,hcalc)
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use mmap_module
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implicit none
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BEGIN_DOC
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@ -412,36 +412,6 @@ subroutine davidson_general_ext_rout(u_in,H_jj,Dress_jj,energies,sze,N_st,N_st_d
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FREE nthreads_davidson
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end
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subroutine hcalc_template(v,u,N_st,sze)
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use bitmasks
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implicit none
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BEGIN_DOC
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! Template of routine for the application of H
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!
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! Here, it is done with the Hamiltonian matrix
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!
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! on the set of determinants of psi_det
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!
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! Computes $v = H | u \rangle$
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!
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END_DOC
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integer, intent(in) :: N_st,sze
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double precision, intent(in) :: u(sze,N_st)
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double precision, intent(inout) :: v(sze,N_st)
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integer :: i,j,istate
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v = 0.d0
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do istate = 1, N_st
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do i = 1, sze
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do j = 1, sze
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v(i,istate) += H_matrix_all_dets(j,i) * u(j,istate)
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enddo
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enddo
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do i = 1, sze
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v(i,istate) += u(i,istate) * nuclear_repulsion
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enddo
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enddo
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end
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subroutine dressing_diag_uv(v,u,dress_diag,N_st,sze)
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implicit none
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BEGIN_DOC
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@ -103,13 +103,17 @@ BEGIN_PROVIDER [ double precision, expected_s2]
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END_PROVIDER
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BEGIN_PROVIDER [ double precision, s2_values, (N_states) ]
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BEGIN_PROVIDER [ double precision, s2_values, (N_states) ]
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&BEGIN_PROVIDER [ double precision, s_values, (N_states) ]
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implicit none
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BEGIN_DOC
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! array of the averaged values of the S^2 operator on the various states
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END_DOC
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integer :: i
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call u_0_S2_u_0(s2_values,psi_coef,n_det,psi_det,N_int,N_states,psi_det_size)
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do i = 1, N_states
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s_values(i) = 0.5d0 *(-1.d0 + dsqrt(1.d0 + 4 * s2_values(i)))
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enddo
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END_PROVIDER
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@ -91,7 +91,19 @@
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enddo
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END_PROVIDER
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BEGIN_PROVIDER[double precision, aos_lapl_in_r_array, (ao_num,n_points_final_grid,3)]
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BEGIN_PROVIDER [double precision, aos_lapl_in_r_array_transp, (ao_num, n_points_final_grid,3)]
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implicit none
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integer :: i,j,m
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do i = 1, n_points_final_grid
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do j = 1, ao_num
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do m = 1, 3
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aos_lapl_in_r_array_transp(j,i,m) = aos_lapl_in_r_array(m,j,i)
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enddo
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enddo
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enddo
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END_PROVIDER
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BEGIN_PROVIDER [double precision, aos_lapl_in_r_array, (3,ao_num,n_points_final_grid)]
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implicit none
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BEGIN_DOC
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! aos_lapl_in_r_array(i,j,k) = value of the kth component of the laplacian of jth ao on the ith grid point
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@ -100,20 +112,20 @@
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END_DOC
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integer :: i,j,m
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double precision :: aos_array(ao_num), r(3)
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double precision :: aos_grad_array(ao_num,3)
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double precision :: aos_lapl_array(ao_num,3)
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double precision :: aos_grad_array(3,ao_num)
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double precision :: aos_lapl_array(3,ao_num)
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!$OMP PARALLEL DO &
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!$OMP DEFAULT (NONE) &
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!$OMP PRIVATE (i,r,aos_array,aos_grad_array,aos_lapl_array,j,m) &
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!$OMP SHARED(aos_lapl_in_r_array,n_points_final_grid,ao_num,final_grid_points)
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do m = 1, 3
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do i = 1, n_points_final_grid
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r(1) = final_grid_points(1,i)
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r(2) = final_grid_points(2,i)
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r(3) = final_grid_points(3,i)
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call give_all_aos_and_grad_and_lapl_at_r(r,aos_array,aos_grad_array,aos_lapl_array)
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do j = 1, ao_num
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aos_lapl_in_r_array(j,i,m) = aos_lapl_array(j,m)
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do i = 1, n_points_final_grid
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r(1) = final_grid_points(1,i)
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r(2) = final_grid_points(2,i)
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r(3) = final_grid_points(3,i)
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call give_all_aos_and_grad_and_lapl_at_r(r,aos_array,aos_grad_array,aos_lapl_array)
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do j = 1, ao_num
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do m = 1, 3
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aos_lapl_in_r_array(m,j,i) = aos_lapl_array(m,j)
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enddo
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enddo
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enddo
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@ -138,7 +138,7 @@
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integer :: m
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mos_lapl_in_r_array = 0.d0
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do m=1,3
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call dgemm('N','N',mo_num,n_points_final_grid,ao_num,1.d0,mo_coef_transp,mo_num,aos_lapl_in_r_array(1,1,m),ao_num,0.d0,mos_lapl_in_r_array(1,1,m),mo_num)
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call dgemm('N','N',mo_num,n_points_final_grid,ao_num,1.d0,mo_coef_transp,mo_num,aos_lapl_in_r_array_transp(1,1,m),ao_num,0.d0,mos_lapl_in_r_array(1,1,m),mo_num)
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enddo
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END_PROVIDER
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@ -7,7 +7,7 @@ subroutine hcore_guess
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label = 'Guess'
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call mo_as_eigvectors_of_mo_matrix(mo_one_e_integrals, &
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size(mo_one_e_integrals,1), &
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size(mo_one_e_integrals,2),label,1,.false.)
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size(mo_one_e_integrals,2),label,1,.true.)
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call nullify_small_elements(ao_num, mo_num, mo_coef, size(mo_coef,1), 1.d-12 )
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call save_mos
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TOUCH mo_coef mo_label
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@ -32,8 +32,9 @@ subroutine routine
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double precision :: norm_mono_a,norm_mono_b
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double precision :: norm_mono_a_2,norm_mono_b_2
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double precision :: norm_mono_a_pert_2,norm_mono_b_pert_2
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double precision :: norm_mono_a_pert,norm_mono_b_pert
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double precision :: norm_mono_a_pert,norm_mono_b_pert,norm_double_1
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double precision :: delta_e,coef_2_2
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norm_mono_a = 0.d0
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norm_mono_b = 0.d0
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norm_mono_a_2 = 0.d0
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@ -42,6 +43,7 @@ subroutine routine
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norm_mono_b_pert = 0.d0
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norm_mono_a_pert_2 = 0.d0
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norm_mono_b_pert_2 = 0.d0
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norm_double_1 = 0.d0
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do i = 1, min(N_det_print_wf,N_det)
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print*,''
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print*,'i = ',i
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@ -93,6 +95,7 @@ subroutine routine
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print*,'h1,p1 = ',h1,p1
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print*,'s2',s2
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print*,'h2,p2 = ',h2,p2
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norm_double_1 += dabs(psi_coef_sorted(i,1)/psi_coef_sorted(1,1))
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endif
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print*,'<Ref| H |D_I> = ',hij
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@ -109,6 +112,7 @@ subroutine routine
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print*,''
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print*,'L1 norm of mono alpha = ',norm_mono_a
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print*,'L1 norm of mono beta = ',norm_mono_b
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print*,'L1 norm of double exc = ',norm_double_1
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print*, '---'
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print*,'L2 norm of mono alpha = ',norm_mono_a_2
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print*,'L2 norm of mono beta = ',norm_mono_b_2
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