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working on second order corrections with multi parentage
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plugins/MRPT_Utils/new_way_second_order_coef.irp.f
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710
plugins/MRPT_Utils/new_way_second_order_coef.irp.f
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subroutine give_2h1p_contrib_sec_order(matrix_2h1p)
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use bitmasks
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implicit none
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double precision , intent(inout) :: matrix_2h1p(N_det,N_det,*)
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integer :: i,j,r,a,b
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integer :: iorb, jorb, rorb, aorb, borb
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integer :: ispin,jspin
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integer :: idet,jdet
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integer(bit_kind) :: perturb_dets(N_int,2,n_act_orb,2,2)
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double precision :: perturb_dets_phase(n_act_orb,2,2)
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double precision :: perturb_dets_hij(n_act_orb,2,2)
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double precision :: coef_perturb_from_idet(n_act_orb,2,2,N_states,3)
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integer :: inint
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integer :: elec_num_tab_local(2),acu_elec
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integer(bit_kind) :: det_tmp(N_int,2)
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integer(bit_kind) :: det_tmp_j(N_int,2)
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integer :: exc(0:2,2,2)
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integer :: accu_elec
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double precision :: get_mo_bielec_integral_schwartz
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double precision :: active_int(n_act_orb,2)
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double precision :: hij,phase
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!matrix_2h1p = 0.d0
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elec_num_tab_local = 0
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do inint = 1, N_int
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elec_num_tab_local(1) += popcnt(psi_det(inint,1,1))
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elec_num_tab_local(2) += popcnt(psi_det(inint,2,1))
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enddo
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do i = 1, n_inact_orb ! First inactive
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iorb = list_inact(i)
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do j = 1, n_inact_orb ! Second inactive
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jorb = list_inact(j)
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do r = 1, n_virt_orb ! First virtual
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rorb = list_virt(r)
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! take all the integral you will need for i,j,r fixed
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do a = 1, n_act_orb
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aorb = list_act(a)
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active_int(a,1) = get_mo_bielec_integral_schwartz(iorb,jorb,rorb,aorb,mo_integrals_map) ! direct
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active_int(a,2) = get_mo_bielec_integral_schwartz(iorb,jorb,aorb,rorb,mo_integrals_map) ! exchange
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perturb_dets_phase(a,1,1) = -1000.d0
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perturb_dets_phase(a,1,2) = -1000.d0
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perturb_dets_phase(a,2,2) = -1000.d0
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perturb_dets_phase(a,2,1) = -1000.d0
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enddo
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integer :: degree(N_det)
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integer :: idx(0:N_det)
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double precision :: delta_e(n_act_orb,2,N_states)
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integer :: istate
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integer :: index_orb_act_mono(N_det,3)
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do idet = 1, N_det
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call get_excitation_degree_vector_mono(psi_det,psi_det(1,1,idet),degree,N_int,N_det,idx)
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!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! Precomputation of matrix elements
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do ispin = 1, 2 ! spin of the couple a-a^dagger (i,r)
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do jspin = 1, 2 ! spin of the couple z-a^dagger (j,a)
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if(ispin == jspin .and. iorb.le.jorb)cycle ! condition not to double count
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do a = 1, n_act_orb ! First active
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aorb = list_act(a)
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do inint = 1, N_int
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det_tmp(inint,1) = psi_det(inint,1,idet)
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det_tmp(inint,2) = psi_det(inint,2,idet)
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enddo
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! Do the excitation inactive -- > virtual
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call clear_bit_to_integer(iorb,det_tmp(1,ispin),N_int) ! hole in "iorb" of spin Ispin
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call set_bit_to_integer(rorb,det_tmp(1,ispin),N_int) ! particle in "rorb" of spin Ispin
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! Do the excitation inactive -- > active
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call clear_bit_to_integer(jorb,det_tmp(1,jspin),N_int) ! hole in "jorb" of spin Jspin
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call set_bit_to_integer(aorb,det_tmp(1,jspin),N_int) ! particle in "aorb" of spin Jspin
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! Check if the excitation is possible or not on psi_det(idet)
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accu_elec= 0
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do inint = 1, N_int
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accu_elec+= popcnt(det_tmp(inint,jspin))
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enddo
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if(accu_elec .ne. elec_num_tab_local(jspin))then
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perturb_dets_phase(a,jspin,ispin) = -1000.d0
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perturb_dets_hij(a,jspin,ispin) = 0.d0
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do istate = 1, N_states
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coef_perturb_from_idet(a,jspin,ispin,istate,1) = 0.d0
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coef_perturb_from_idet(a,jspin,ispin,istate,2) = 0.d0
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enddo
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cycle
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endif
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do inint = 1, N_int
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perturb_dets(inint,1,a,jspin,ispin) = det_tmp(inint,1)
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perturb_dets(inint,2,a,jspin,ispin) = det_tmp(inint,2)
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enddo
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call get_double_excitation(psi_det(1,1,idet),det_tmp,exc,phase,N_int)
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perturb_dets_phase(a,jspin,ispin) = phase
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do istate = 1, N_states
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delta_e(a,jspin,istate) = one_creat(a,jspin,istate) &
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- fock_virt_total_spin_trace(rorb,istate) &
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+ fock_core_inactive_total_spin_trace(iorb,istate) &
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+ fock_core_inactive_total_spin_trace(jorb,istate)
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enddo
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if(ispin == jspin)then
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perturb_dets_hij(a,jspin,ispin) = phase * (active_int(a,2) - active_int(a,1) )
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else
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perturb_dets_hij(a,jspin,ispin) = phase * active_int(a,1)
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endif
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!!!!!!!!!!!!!!!!!!!!!1 Computation of the coefficient at first order coming from idet
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!!!!!!!!!!!!!!!!!!!!! for the excitation (i,j)(ispin,jspin) ---> (r,a)(ispin,jspin)
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do istate = 1, N_states
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coef_perturb_from_idet(a,jspin,ispin,istate,1) = perturb_dets_hij(a,jspin,ispin) / delta_e(a,jspin,istate)
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enddo
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enddo
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enddo
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enddo
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!!!!!!!!!!!!!!!!!!!!!!!!!!!! Second order coefficient : interactions between the perturbers throw the active space
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do a = 1, n_act_orb
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do jspin = 1, 2
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do ispin = 1, 2
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if( perturb_dets_phase(a,jspin,ispin) .le. -10.d0)cycle
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! determinant perturber | det_tmp > = a^{\dagger}_{r,ispin} a^{\dagger}_{v,jspin} a_{a,jspin} a_{i,ispin} | Idet >
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do inint = 1, N_int
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det_tmp(inint,1) = iand(perturb_dets(inint,1,a,jspin,ispin),cas_bitmask(inint,1,1))
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det_tmp(inint,2) = iand(perturb_dets(inint,2,a,jspin,ispin),cas_bitmask(inint,1,1))
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enddo
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do istate = 1, N_states
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coef_perturb_from_idet(a,jspin,ispin,istate,2) = 0.d0
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enddo
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do b = 1, n_act_orb
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do kspin = jspin , jspin
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integer :: degree_scalar
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if( perturb_dets_phase(b,kspin,ispin) .le. -10.d0)cycle
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do inint = 1, N_int
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det_tmp_j(inint,1) = iand(perturb_dets(inint,1,b,kspin,ispin),cas_bitmask(inint,1,1))
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det_tmp_j(inint,2) = iand(perturb_dets(inint,2,b,kspin,ispin),cas_bitmask(inint,1,1))
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enddo
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call get_excitation_degree(det_tmp,det_tmp_j,degree_scalar,N_int)
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if (degree_scalar > 2 .or. degree_scalar == 0)cycle
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! determinant perturber | det_tmp_j > = a^{\dagger}_{r,ispin} a^{\dagger}_{v,jspin} a_{b,jspin} a_{i,ispin} | Idet >
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! print*, '**********************'
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! integer(bit_kind) :: det_bis(N_int,2)
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! call debug_det(det_tmp,N_int)
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! call debug_det(det_tmp_j,N_int)
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! do inint = 1, N_int
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! det_bis(inint,1) = perturb_dets(inint,1,b,kspin,ispin)
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! det_bis(inint,2) = perturb_dets(inint,2,b,kspin,ispin)
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! enddo
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! call debug_det(det_bis,N_int)
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call i_H_j_dyall(det_tmp,det_tmp_j,N_int,hij)
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do istate = 1, N_states
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coef_perturb_from_idet(a,jspin,ispin,istate,2) += coef_perturb_from_idet(b,kspin,ispin,istate,1) &
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* hij / delta_e(a,jspin,istate)
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if(dabs(hij).gt.0.01d0)then
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print*,degree_scalar, hij
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print*, coef_perturb_from_idet(b,kspin,ispin,istate,1)* hij / delta_e(a,jspin,istate),coef_perturb_from_idet(a,jspin,ispin,istate,1)
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endif
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enddo
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enddo
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enddo
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enddo
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enddo
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enddo
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do a = 1, n_act_orb
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do jspin = 1, 2
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do ispin = 1, 2
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if( perturb_dets_phase(a,jspin,ispin) .le. -10.d0)cycle
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do istate = 1, N_states
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! print*, coef_perturb_from_idet(a,jspin,ispin,istate,1),coef_perturb_from_idet(a,jspin,ispin,istate,2)
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coef_perturb_from_idet(a,jspin,ispin,istate,2) += coef_perturb_from_idet(a,jspin,ispin,istate,1)
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enddo
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enddo
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enddo
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enddo
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! stop
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!!!!!!!!!!!!!!!!!!!!!!!!!!! determination of the connections between I and the other J determinants mono excited in the CAS
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!!!!!!!!!!!!!!!!!!!!!!!!!!!! the determinants I and J must be connected by the following operator
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!!!!!!!!!!!!!!!!!!!!!!!!!!!! <Jdet | a_{b} a^{\dagger}_a | Idet>
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do jdet = 1, idx(0)
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if(idx(jdet).ne.idet)then
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call get_mono_excitation(psi_det(1,1,idet),psi_det(1,1,idx(jdet)),exc,phase,N_int)
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if (exc(0,1,1) == 1) then
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! Mono alpha
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index_orb_act_mono(idx(jdet),1) = list_act_reverse(exc(1,2,1)) !!! a^{\dagger}_a
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index_orb_act_mono(idx(jdet),2) = list_act_reverse(exc(1,1,1)) !!! a_{b}
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index_orb_act_mono(idx(jdet),3) = 1
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else
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! Mono beta
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index_orb_act_mono(idx(jdet),1) = list_act_reverse(exc(1,2,2)) !!! a^{\dagger}_a
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index_orb_act_mono(idx(jdet),2) = list_act_reverse(exc(1,1,2)) !!! a_{b}
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index_orb_act_mono(idx(jdet),3) = 2
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endif
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else
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index_orb_act_mono(idx(jdet),1) = -1
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endif
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enddo
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integer :: kspin
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do jdet = 1, idx(0)
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if(idx(jdet).ne.idet)then
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! two determinants | Idet > and | Jdet > which are connected throw a mono excitation operator
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! are connected by the presence of the perturbers determinants |det_tmp>
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aorb = index_orb_act_mono(idx(jdet),1) ! a^{\dagger}_{aorb}
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borb = index_orb_act_mono(idx(jdet),2) ! a_{borb}
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kspin = index_orb_act_mono(idx(jdet),3) ! spin of the excitation
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! the determinants Idet and Jdet interact throw the following operator
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! | Jdet > = a_{borb,kspin} a^{\dagger}_{aorb, kspin} | Idet >
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do ispin = 1, 2 ! you loop on all possible spin for the excitation
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! a^{\dagger}_r a_{i} (ispin)
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if(ispin == kspin .and. iorb.le.jorb)cycle ! condition not to double count
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! | det_tmp > = a^{\dagger}_{rorb,ispin} a^{\dagger}_{aorb,kspin} a_{jorb,kspin} a_{iorb,ispin} | Idet >
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do inint = 1, N_int
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det_tmp(inint,1) = perturb_dets(inint,1,aorb,kspin,ispin)
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det_tmp(inint,2) = perturb_dets(inint,2,aorb,kspin,ispin)
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enddo
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double precision :: hja
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! you determine the interaction between the excited determinant and the other parent | Jdet >
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! | det_tmp > = a^{\dagger}_{rorb,ispin} a^{\dagger}_{borb,kspin} a_{jorb,kspin} a_{iorb,ispin} | Jdet >
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! hja = < det_tmp | H | Jdet >
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call get_double_excitation(psi_det(1,1,idx(jdet)),det_tmp,exc,phase,N_int)
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if(kspin == ispin)then
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hja = phase * (active_int(borb,2) - active_int(borb,1) )
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else
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hja = phase * active_int(borb,1)
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endif
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do istate = 1, N_states
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matrix_2h1p(idx(jdet),idet,istate) += hja * coef_perturb_from_idet(aorb,kspin,ispin,istate,2)
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enddo
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enddo ! ispin
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else
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! diagonal part of the dressing : interaction of | Idet > with all the perturbers generated by the excitations
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!
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! | det_tmp > = a^{\dagger}_{rorb,ispin} a^{\dagger}_{aorb,kspin} a_{jorb,kspin} a_{iorb,ispin} | Idet >
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do ispin = 1, 2
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do kspin = 1, 2
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if(ispin == kspin .and. iorb.le.jorb)cycle ! condition not to double count
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do a = 1, n_act_orb ! First active
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do istate = 1, N_states
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matrix_2h1p(idet,idet,istate) += coef_perturb_from_idet(a,kspin,ispin,istate,2) * perturb_dets_hij(a,kspin,ispin)
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enddo
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enddo
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enddo
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enddo
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endif
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enddo
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enddo
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enddo
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enddo
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enddo
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end
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subroutine give_1h2p_contrib_sec_order(matrix_1h2p)
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use bitmasks
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implicit none
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double precision , intent(inout) :: matrix_1h2p(N_det,N_det,*)
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integer :: i,v,r,a,b
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integer :: iorb, vorb, rorb, aorb, borb
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integer :: ispin,jspin
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integer :: idet,jdet
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integer(bit_kind) :: perturb_dets(N_int,2,n_act_orb,2,2)
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double precision :: perturb_dets_phase(n_act_orb,2,2)
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double precision :: perturb_dets_hij(n_act_orb,2,2)
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double precision :: perturb_dets_hpsi0(n_act_orb,2,2,N_states)
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double precision :: coef_perturb_from_idet(n_act_orb,2,2,N_states,2)
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logical :: already_generated(n_act_orb,2,2)
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integer :: inint
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integer :: elec_num_tab_local(2),acu_elec
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integer(bit_kind) :: det_tmp(N_int,2)
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integer(bit_kind) :: det_tmp_j(N_int,2)
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integer :: exc(0:2,2,2)
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integer :: accu_elec
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double precision :: get_mo_bielec_integral_schwartz
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double precision :: active_int(n_act_orb,2)
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double precision :: hij,phase
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double precision :: accu_contrib
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integer :: degree(N_det)
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integer :: idx(0:N_det)
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double precision :: delta_e(n_act_orb,2,N_states)
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integer :: istate
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integer :: index_orb_act_mono(N_det,6)
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double precision :: delta_e_inactive_virt(N_states)
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integer :: kspin
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double precision :: delta_e_ja(N_states)
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double precision :: hja
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double precision :: contrib_hij
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accu_contrib = 0.d0
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!matrix_1h2p = 0.d0
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elec_num_tab_local = 0
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do inint = 1, N_int
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elec_num_tab_local(1) += popcnt(psi_det(inint,1,1))
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elec_num_tab_local(2) += popcnt(psi_det(inint,2,1))
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enddo
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do i = 1, n_inact_orb ! First inactive
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iorb = list_inact(i)
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do v = 1, n_virt_orb ! First virtual
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vorb = list_virt(v)
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do r = 1, n_virt_orb ! Second virtual
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rorb = list_virt(r)
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! take all the integral you will need for i,j,r fixed
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do a = 1, n_act_orb
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aorb = list_act(a)
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active_int(a,1) = get_mo_bielec_integral_schwartz(iorb,aorb,rorb,vorb,mo_integrals_map) ! direct
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active_int(a,2) = get_mo_bielec_integral_schwartz(iorb,aorb,vorb,rorb,mo_integrals_map) ! exchange
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perturb_dets_phase(a,1,1) = -1000.d0
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perturb_dets_phase(a,1,2) = -1000.d0
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perturb_dets_phase(a,2,2) = -1000.d0
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perturb_dets_phase(a,2,1) = -1000.d0
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already_generated(a,1,1) = .False.
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already_generated(a,1,2) = .False.
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already_generated(a,2,2) = .False.
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already_generated(a,2,1) = .False.
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enddo
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do istate = 1, N_states
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delta_e_inactive_virt(istate) = &
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- fock_virt_total_spin_trace(rorb,istate) &
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- fock_virt_total_spin_trace(vorb,istate) &
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+ fock_core_inactive_total_spin_trace(iorb,istate)
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enddo
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do idet = 1, N_det
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call get_excitation_degree_vector_mono_or_exchange(psi_det,psi_det(1,1,idet),degree,N_int,N_det,idx)
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!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! Precomputation of matrix elements
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do ispin = 1, 2 ! spin of the couple a-a^dagger (iorb,rorb)
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do jspin = 1, 2 ! spin of the couple a-a^dagger (aorb,vorb)
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do a = 1, n_act_orb ! First active
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aorb = list_act(a)
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do istate = 1, N_states
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perturb_dets_hpsi0(a,jspin,ispin,istate) = 0.d0
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coef_perturb_from_idet(a,jspin,ispin,istate,1) = 0.d0
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coef_perturb_from_idet(a,jspin,ispin,istate,2) = 0.d0
|
||||
enddo
|
||||
if(ispin == jspin .and. vorb.le.rorb)cycle ! condition not to double count
|
||||
do inint = 1, N_int
|
||||
det_tmp(inint,1) = psi_det(inint,1,idet)
|
||||
det_tmp(inint,2) = psi_det(inint,2,idet)
|
||||
enddo
|
||||
! Do the excitation inactive -- > virtual
|
||||
call clear_bit_to_integer(iorb,det_tmp(1,ispin),N_int) ! hole in "iorb" of spin Ispin
|
||||
call set_bit_to_integer(rorb,det_tmp(1,ispin),N_int) ! particle in "rorb" of spin Ispin
|
||||
|
||||
! Do the excitation active -- > virtual
|
||||
call clear_bit_to_integer(aorb,det_tmp(1,jspin),N_int) ! hole in "aorb" of spin Jspin
|
||||
call set_bit_to_integer(vorb,det_tmp(1,jspin),N_int) ! particle in "vorb" of spin Jspin
|
||||
|
||||
! Check if the excitation is possible or not on psi_det(idet)
|
||||
accu_elec= 0
|
||||
do inint = 1, N_int
|
||||
accu_elec+= popcnt(det_tmp(inint,jspin))
|
||||
enddo
|
||||
if(accu_elec .ne. elec_num_tab_local(jspin))then
|
||||
perturb_dets_phase(a,jspin,ispin) = -1000.0d0
|
||||
perturb_dets_hij(a,jspin,ispin) = 0.d0
|
||||
do istate = 1, N_states
|
||||
coef_perturb_from_idet(a,jspin,ispin,istate,1) = 0.d0
|
||||
coef_perturb_from_idet(a,jspin,ispin,istate,2) = 0.d0
|
||||
enddo
|
||||
cycle
|
||||
endif
|
||||
do inint = 1, N_int
|
||||
perturb_dets(inint,1,a,jspin,ispin) = det_tmp(inint,1)
|
||||
perturb_dets(inint,2,a,jspin,ispin) = det_tmp(inint,2)
|
||||
enddo
|
||||
do inint = 1, N_int
|
||||
det_tmp(inint,1) = perturb_dets(inint,1,a,jspin,ispin)
|
||||
det_tmp(inint,2) = perturb_dets(inint,2,a,jspin,ispin)
|
||||
enddo
|
||||
|
||||
call get_double_excitation(psi_det(1,1,idet),det_tmp,exc,phase,N_int)
|
||||
perturb_dets_phase(a,jspin,ispin) = phase
|
||||
|
||||
do istate = 1, N_states
|
||||
delta_e(a,jspin,istate) = one_anhil(a,jspin,istate) + delta_e_inactive_virt(istate)
|
||||
enddo
|
||||
if(ispin == jspin)then
|
||||
perturb_dets_hij(a,jspin,ispin) = phase * (active_int(a,1) - active_int(a,2) )
|
||||
else
|
||||
perturb_dets_hij(a,jspin,ispin) = phase * active_int(a,1)
|
||||
endif
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
|
||||
!!!!!!!!!!!!!!!!!!!!!!!!!!! determination of the connections between I and the other J determinants mono excited in the CAS
|
||||
!!!!!!!!!!!!!!!!!!!!!!!!!!!! the determinants I and J must be connected by the following operator
|
||||
!!!!!!!!!!!!!!!!!!!!!!!!!!!! <Jdet | a^{\dagger}_b a_{a} | Idet>
|
||||
do jdet = 1, idx(0)
|
||||
if(idx(jdet).ne.idet)then
|
||||
! print*, degree(jdet)
|
||||
if(degree(jdet)==1)then
|
||||
call get_mono_excitation(psi_det(1,1,idet),psi_det(1,1,idx(jdet)),exc,phase,N_int)
|
||||
if (exc(0,1,1) == 1) then
|
||||
! Mono alpha
|
||||
index_orb_act_mono(idx(jdet),1) = list_act_reverse(exc(1,1,1)) !!! a_a
|
||||
index_orb_act_mono(idx(jdet),2) = list_act_reverse(exc(1,2,1)) !!! a^{\dagger}_{b}
|
||||
index_orb_act_mono(idx(jdet),3) = 1
|
||||
else
|
||||
! Mono beta
|
||||
index_orb_act_mono(idx(jdet),1) = list_act_reverse(exc(1,1,2)) !!! a_a
|
||||
index_orb_act_mono(idx(jdet),2) = list_act_reverse(exc(1,2,2)) !!! a^{\dagger}_{b}
|
||||
index_orb_act_mono(idx(jdet),3) = 2
|
||||
endif
|
||||
else if(degree(jdet)==2)then
|
||||
call get_double_excitation(psi_det(1,1,idet),psi_det(1,1,idx(jdet)),exc,phase,N_int)
|
||||
! Mono alpha
|
||||
index_orb_act_mono(idx(jdet),1) = list_act_reverse(exc(1,1,1)) !!! a_a
|
||||
index_orb_act_mono(idx(jdet),2) = list_act_reverse(exc(1,2,1)) !!! a^{\dagger}_{b}
|
||||
index_orb_act_mono(idx(jdet),3) = 1
|
||||
! Mono beta
|
||||
index_orb_act_mono(idx(jdet),4) = list_act_reverse(exc(1,1,2)) !!! a_a
|
||||
index_orb_act_mono(idx(jdet),5) = list_act_reverse(exc(1,2,2)) !!! a^{\dagger}_{b}
|
||||
index_orb_act_mono(idx(jdet),6) = 2
|
||||
! print*, '******************'
|
||||
! call debug_det(psi_det(1,1,idet),N_int)
|
||||
! call debug_det(psi_det(1,1,idx(jdet)),N_int)
|
||||
! print*, 'h1,p1,s1 = ',index_orb_act_mono(idx(jdet),1),index_orb_act_mono(idx(jdet),2), index_orb_act_mono(idx(jdet),3)
|
||||
! print*, 'h2,p2,s2 = ',index_orb_act_mono(idx(jdet),4),index_orb_act_mono(idx(jdet),5), index_orb_act_mono(idx(jdet),6)
|
||||
! print*, '******************'
|
||||
! pause
|
||||
endif
|
||||
else
|
||||
index_orb_act_mono(idx(jdet),1) = -1
|
||||
endif
|
||||
enddo
|
||||
|
||||
|
||||
|
||||
do jdet = 1, idx(0)
|
||||
if(idx(jdet).ne.idet)then
|
||||
if(degree(jdet) == 1)then
|
||||
! two determinants | Idet > and | Jdet > which are connected throw a mono excitation operator
|
||||
! are connected by the presence of the perturbers determinants |det_tmp>
|
||||
aorb = index_orb_act_mono(idx(jdet),1) ! a_{aorb}
|
||||
borb = index_orb_act_mono(idx(jdet),2) ! a^{\dagger}_{borb}
|
||||
kspin = index_orb_act_mono(idx(jdet),3) ! spin of the excitation
|
||||
! the determinants Idet and Jdet interact throw the following operator
|
||||
! | Jdet > = a^{\dagger}_{borb,kspin} a_{aorb, kspin} | Idet >
|
||||
|
||||
do ispin = 1, 2 ! you loop on all possible spin for the excitation
|
||||
! a^{\dagger}_r a_{i} (ispin)
|
||||
integer ::corb,dorb,i_ok
|
||||
integer(bit_kind) :: det_tmp_bis(N_int,2)
|
||||
double precision :: hib , hab
|
||||
double precision :: delta_e_ab(N_states)
|
||||
double precision :: hib_test,hja_test,hab_test
|
||||
if(ispin == kspin .and. vorb.le.rorb)cycle ! condition not to double count
|
||||
do jspin = 1, 2
|
||||
if (jspin .ne. kspin)then
|
||||
do corb = 1, n_act_orb
|
||||
if(perturb_dets_phase(corb,jspin,ispin).le.-100d0)cycle
|
||||
! | det_tmp > = a^{\dagger}_{rorb,ispin} a^{\dagger}_{vorb,kspin} a_{corb,kspin} a_{iorb,ispin} | Idet >
|
||||
do inint = 1, N_int
|
||||
det_tmp(inint,1) = perturb_dets(inint,1,corb,jspin,ispin)
|
||||
det_tmp(inint,2) = perturb_dets(inint,2,corb,jspin,ispin)
|
||||
det_tmp_bis(inint,1) = perturb_dets(inint,1,corb,jspin,ispin)
|
||||
det_tmp_bis(inint,2) = perturb_dets(inint,2,corb,jspin,ispin)
|
||||
enddo
|
||||
! < idet | H | det_tmp > = phase * (ir|cv)
|
||||
! call i_H_j(det_tmp,psi_det(1,1,idet),N_int,hib)
|
||||
call get_double_excitation(psi_det(1,1,idet),det_tmp,exc,phase,N_int)
|
||||
if(ispin == jspin)then
|
||||
hib= phase * (active_int(corb,1) - active_int(corb,2))
|
||||
else
|
||||
hib= phase * active_int(corb,1)
|
||||
endif
|
||||
! if(hib_test .ne. hib)then
|
||||
! print*, 'hib_test .ne. hib'
|
||||
! print*, hib, hib_test
|
||||
! stop
|
||||
! endif
|
||||
|
||||
! | det_tmp_bis > = a^{\dagger}_{borb,kspin} a_{aorb,kspin} | det_tmp >
|
||||
call do_mono_excitation(det_tmp_bis,list_act(aorb),list_act(borb),kspin,i_ok)
|
||||
if(i_ok .ne. 1)cycle
|
||||
|
||||
! < det_tmp | H | det_tmp_bis > = F_{aorb,borb}
|
||||
call i_H_j(det_tmp_bis,det_tmp,N_int,hab)
|
||||
! < jdet | H | det_tmp_bis > = phase * (ir|cv)
|
||||
! call i_H_j(det_tmp_bis,psi_det(1,1,idx(jdet)),N_int,hja)
|
||||
call get_double_excitation(det_tmp_bis,psi_det(1,1,idx(jdet)),exc,phase,N_int)
|
||||
if(ispin == jspin)then
|
||||
hja= phase * (active_int(corb,1) - active_int(corb,2))
|
||||
else
|
||||
hja= phase * (active_int(corb,1))
|
||||
endif
|
||||
! if(hja_test .ne. hja)then
|
||||
! print*, 'hja_test .ne. hja'
|
||||
! print*, hja, hja_test
|
||||
! stop
|
||||
! endif
|
||||
do istate = 1, N_states
|
||||
delta_e_ab(istate) = delta_e(corb,jspin,istate) + one_anhil_one_creat(borb,aorb,kspin,kspin,istate)
|
||||
matrix_1h2p(idx(jdet),idet,istate) = matrix_1h2p(idx(jdet),idet,istate) + &
|
||||
hib / delta_e(corb,jspin,istate) * hab / delta_e_ab(istate) * hja
|
||||
! < det_tmp | H | Idet > / delta_E (Idet --> det_tmp )
|
||||
! < det_tmp | H | det_tmp_bis > / delta_E (Idet --> det_tmp --> det_tmp_bis)
|
||||
! < det_tmp_bis | H | Jdet >
|
||||
enddo
|
||||
enddo ! corb
|
||||
else
|
||||
do corb = 1, n_act_orb
|
||||
if(corb == aorb .or. corb == borb) cycle
|
||||
if(perturb_dets_phase(corb,jspin,ispin).le.-100d0)cycle
|
||||
! | det_tmp > = a^{\dagger}_{rorb,ispin} a^{\dagger}_{vorb,kspin} a_{corb,kspin} a_{iorb,ispin} | Idet >
|
||||
do inint = 1, N_int
|
||||
det_tmp(inint,1) = perturb_dets(inint,1,corb,jspin,ispin)
|
||||
det_tmp(inint,2) = perturb_dets(inint,2,corb,jspin,ispin)
|
||||
det_tmp_bis(inint,1) = perturb_dets(inint,1,corb,jspin,ispin)
|
||||
det_tmp_bis(inint,2) = perturb_dets(inint,2,corb,jspin,ispin)
|
||||
enddo
|
||||
! < idet | H | det_tmp > = phase * ( (ir|cv) - (iv|cr) )
|
||||
! call i_H_j(det_tmp,psi_det(1,1,idet),N_int,hib)
|
||||
call get_double_excitation(psi_det(1,1,idet),det_tmp,exc,phase,N_int)
|
||||
if(ispin == jspin)then
|
||||
hib= phase * (active_int(corb,1) - active_int(corb,2))
|
||||
else
|
||||
hib= phase * active_int(corb,1)
|
||||
endif
|
||||
! if(hib_test .ne. hib)then
|
||||
! print*, 'hib_test .ne. hib jspin == kspin'
|
||||
! print*, hib, hib_test
|
||||
! stop
|
||||
! endif
|
||||
! | det_tmp_bis > = a^{\dagger}_{borb,kspin} a_{aorb,kspin} | det_tmp >
|
||||
call do_mono_excitation(det_tmp_bis,list_act(aorb),list_act(borb),kspin,i_ok)
|
||||
if(i_ok .ne. 1)cycle
|
||||
! ! < det_tmp | H | det_tmp_bis > = F_{aorb,borb}
|
||||
call i_H_j(det_tmp_bis,det_tmp,N_int,hab)
|
||||
! < jdet | H | det_tmp_bis > = phase * ( (ir|cv) - (iv|cr) )
|
||||
! call i_H_j(det_tmp_bis,psi_det(1,1,idx(jdet)),N_int,hja)
|
||||
call get_double_excitation(det_tmp_bis,psi_det(1,1,idx(jdet)),exc,phase,N_int)
|
||||
if(ispin == jspin)then
|
||||
hja= phase * (active_int(corb,1) - active_int(corb,2))
|
||||
else
|
||||
hja= phase * (active_int(corb,1))
|
||||
endif
|
||||
! if(hja_test .ne. hja)then
|
||||
! print*, 'hja_test .ne. hja'
|
||||
! print*, hja, hja_test
|
||||
! stop
|
||||
! endif
|
||||
do istate = 1, N_states
|
||||
delta_e_ab(istate) = delta_e(corb,jspin,istate) + one_anhil_one_creat(borb,aorb,kspin,kspin,istate)
|
||||
matrix_1h2p(idx(jdet),idet,istate) = matrix_1h2p(idx(jdet),idet,istate) + &
|
||||
hib / delta_e(corb,jspin,istate) * hab / delta_e_ab(istate) * hja
|
||||
! < det_tmp | H | Idet > / delta_E (Idet --> det_tmp )
|
||||
! < det_tmp | H | det_tmp_bis > / delta_E (Idet --> det_tmp --> det_tmp_bis)
|
||||
! < det_tmp_bis | H | Jdet >
|
||||
enddo
|
||||
enddo ! corb
|
||||
|
||||
endif
|
||||
enddo ! jspin
|
||||
enddo ! ispin
|
||||
else
|
||||
!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! Case of double excitations !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!
|
||||
! call debug_det(psi_det(1,1,idet),N_int)
|
||||
! call debug_det(psi_det(1,1,idx(jdet)),N_int)
|
||||
! pause
|
||||
|
||||
|
||||
endif
|
||||
|
||||
else
|
||||
! diagonal part of the dressing : interaction of | Idet > with all the perturbers generated by the excitations
|
||||
!
|
||||
! | det_tmp > = a^{\dagger}_{rorb,ispin} a^{\dagger}_{vorb,kspin} a_{aorb,kspin} a_{iorb,ispin} | Idet >
|
||||
do ispin = 1, 2
|
||||
do kspin = 1, 2
|
||||
do a = 1, n_act_orb ! First active
|
||||
if( perturb_dets_phase(a,kspin,ispin) .le. -10.d0)cycle
|
||||
if(ispin == kspin .and. vorb.le.rorb)cycle ! condition not to double count
|
||||
contrib_hij = perturb_dets_hij(a,kspin,ispin) * perturb_dets_hij(a,kspin,ispin)
|
||||
do istate = 1, N_states
|
||||
! matrix_1h2p(idet,idet,istate) += contrib_hij * delta_e(a,kspin,istate)
|
||||
! perturb_dets_hpsi0(a,kspin,ispin,istate) += psi_coef(idet,istate) * perturb_dets_hij(a,kspin,ispin)
|
||||
! coef_perturb_from_idet(a,kspin,ispin,istate,1) += psi_coef(idet,istate) &
|
||||
! * perturb_dets_hij(a,kspin,ispin) * delta_e(a,kspin,istate)
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
|
||||
endif
|
||||
|
||||
enddo
|
||||
|
||||
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
print* , 'accu_contrib = ',accu_contrib
|
||||
|
||||
|
||||
|
||||
|
||||
|
||||
end
|
||||
|
||||
|
||||
|
||||
|
||||
|
||||
|
||||
|
||||
! do a = 1, n_act_orb
|
||||
! do jspin = 1, 2
|
||||
! do ispin = 1, 2
|
||||
! if( perturb_dets_phase(a,jspin,ispin) .le. -10.d0)cycle
|
||||
! ! determinant perturber | det_tmp > = a^{\dagger}_{r,ispin} a^{\dagger}_{v,jspin} a_{a,jspin} a_{i,ispin} | Idet >
|
||||
! do inint = 1, N_int
|
||||
! det_tmp(inint,1) = perturb_dets(inint,1,a,jspin,ispin)
|
||||
! det_tmp(inint,2) = perturb_dets(inint,2,a,jspin,ispin)
|
||||
! enddo
|
||||
! do istate = 1, N_states
|
||||
! coef_perturb_from_idet(a,jspin,ispin,istate,2) = 0.d0
|
||||
! enddo
|
||||
! do b = 1, n_act_orb
|
||||
! do kspin = jspin , jspin
|
||||
! integer :: degree_scalar
|
||||
! if( perturb_dets_phase(b,kspin,ispin) .le. -10.d0)cycle
|
||||
! do inint = 1, N_int
|
||||
! det_tmp_j(inint,1) = perturb_dets(inint,1,b,kspin,ispin)
|
||||
! det_tmp_j(inint,2) = perturb_dets(inint,2,b,kspin,ispin)
|
||||
! enddo
|
||||
! call get_excitation_degree(det_tmp,det_tmp_j,degree_scalar,N_int)
|
||||
! if (degree_scalar > 2 .or. degree_scalar == 0)cycle
|
||||
! ! determinant perturber | det_tmp_j > = a^{\dagger}_{r,ispin} a^{\dagger}_{v,jspin} a_{b,jspin} a_{i,ispin} | Idet >
|
||||
! call i_H_j(det_tmp,det_tmp_j,N_int,hij)
|
||||
! do istate = 1, N_states
|
||||
! coef_perturb_from_idet(a,jspin,ispin,istate,2) += coef_perturb_from_idet(b,kspin,ispin,istate,1) &
|
||||
! * hij / delta_e(a,jspin,istate)
|
||||
! endif
|
||||
! enddo
|
||||
! enddo
|
||||
! enddo
|
||||
! enddo
|
||||
! enddo
|
||||
! enddo
|
||||
|
||||
|
||||
|
||||
! do a = 1, n_act_orb
|
||||
! do jspin = 1, 2
|
||||
! do ispin = 1, 2
|
||||
! if( perturb_dets_phase(a,jspin,ispin) .le. -10.d0)cycle
|
||||
! ! determinant perturber | det_tmp > = a^{\dagger}_{r,ispin} a^{\dagger}_{v,jspin} a_{a,jspin} a_{i,ispin} | Idet >
|
||||
! do inint = 1, N_int
|
||||
! det_tmp(inint,1) = iand(perturb_dets(inint,1,a,jspin,ispin),cas_bitmask(inint,1,1))
|
||||
! det_tmp(inint,2) = iand(perturb_dets(inint,2,a,jspin,ispin),cas_bitmask(inint,1,1))
|
||||
! enddo
|
||||
! do istate = 1, N_states
|
||||
! coef_perturb_from_idet(a,jspin,ispin,istate,2) = 0.d0
|
||||
! enddo
|
||||
! do b = 1, n_act_orb
|
||||
! do kspin = jspin , jspin
|
||||
! integer :: degree_scalar
|
||||
! if( perturb_dets_phase(b,kspin,ispin) .le. -10.d0)cycle
|
||||
! do inint = 1, N_int
|
||||
! det_tmp_j(inint,1) = iand(perturb_dets(inint,1,b,kspin,ispin),cas_bitmask(inint,1,1))
|
||||
! det_tmp_j(inint,2) = iand(perturb_dets(inint,2,b,kspin,ispin),cas_bitmask(inint,1,1))
|
||||
! enddo
|
||||
! call get_excitation_degree(det_tmp,det_tmp_j,degree_scalar,N_int)
|
||||
! if (degree_scalar > 2 .or. degree_scalar == 0)cycle
|
||||
! ! determinant perturber | det_tmp_j > = a^{\dagger}_{r,ispin} a^{\dagger}_{v,jspin} a_{b,jspin} a_{i,ispin} | Idet >
|
||||
!! print*, '**********************'
|
||||
!! integer(bit_kind) :: det_bis(N_int,2)
|
||||
!! call debug_det(det_tmp,N_int)
|
||||
!! call debug_det(det_tmp_j,N_int)
|
||||
!! do inint = 1, N_int
|
||||
!! det_bis(inint,1) = perturb_dets(inint,1,b,kspin,ispin)
|
||||
!! det_bis(inint,2) = perturb_dets(inint,2,b,kspin,ispin)
|
||||
!! enddo
|
||||
!! call debug_det(det_bis,N_int)
|
||||
! call i_H_j_dyall(det_tmp,det_tmp_j,N_int,hij)
|
||||
! do istate = 1, N_states
|
||||
! coef_perturb_from_idet(a,jspin,ispin,istate,2) += coef_perturb_from_idet(b,kspin,ispin,istate,1) &
|
||||
! * hij / delta_e(a,jspin,istate)
|
||||
! if(dabs(hij).gt.0.01d0)then
|
||||
! print*,degree_scalar, hij
|
||||
! print*, coef_perturb_from_idet(b,kspin,ispin,istate,1)* hij / delta_e(a,jspin,istate),coef_perturb_from_idet(a,jspin,ispin,istate,1)
|
||||
!
|
||||
! endif
|
||||
! enddo
|
||||
! enddo
|
||||
! enddo
|
||||
! enddo
|
||||
! enddo
|
||||
! enddo
|
||||
|
||||
! do a = 1, n_act_orb
|
||||
! do jspin = 1, 2
|
||||
! do ispin = 1, 2
|
||||
! if( perturb_dets_phase(a,jspin,ispin) .le. -10.d0)cycle
|
||||
! do istate = 1, N_states
|
||||
! coef_perturb_from_idet(a,jspin,ispin,istate,2) += coef_perturb_from_idet(a,jspin,ispin,istate,1)
|
||||
! enddo
|
||||
! enddo
|
||||
! enddo
|
||||
! enddo
|
31
plugins/MRPT_Utils/print_1h2p.irp.f
Normal file
31
plugins/MRPT_Utils/print_1h2p.irp.f
Normal file
|
@ -0,0 +1,31 @@
|
|||
program print_1h2p
|
||||
implicit none
|
||||
read_wf = .True.
|
||||
touch read_wf
|
||||
call routine
|
||||
end
|
||||
|
||||
subroutine routine
|
||||
implicit none
|
||||
double precision,allocatable :: matrix_1h2p(:,:,:)
|
||||
allocate (matrix_1h2p(N_det,N_det,N_states))
|
||||
integer :: i,j,istate
|
||||
do i = 1, N_det
|
||||
do j = 1, N_det
|
||||
do istate = 1, N_states
|
||||
matrix_1h2p(i,j,istate) = 0.d0
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
call give_1h2p_contrib_sec_order(matrix_1h2p)
|
||||
double precision :: accu
|
||||
accu = 0.d0
|
||||
do i = 1, N_det
|
||||
do j = 1, N_det
|
||||
accu += matrix_1h2p(i,j,1) * psi_coef(i,1) * psi_coef(j,1)
|
||||
enddo
|
||||
enddo
|
||||
print*, 'accu', accu
|
||||
|
||||
deallocate (matrix_1h2p)
|
||||
end
|
|
@ -31,6 +31,8 @@ subroutine do_mono_excitation(key_in,i_hole,i_particle,ispin,i_ok)
|
|||
n_elec_tmp += popcnt(key_in(i,1)) + popcnt(key_in(i,2))
|
||||
enddo
|
||||
if(n_elec_tmp .ne. elec_num)then
|
||||
print*, n_elec_tmp,elec_num
|
||||
call debug_det(key_in,N_int)
|
||||
i_ok = -1
|
||||
endif
|
||||
end
|
||||
|
|
|
@ -1341,6 +1341,162 @@ subroutine get_excitation_degree_vector_mono(key1,key2,degree,Nint,sze,idx)
|
|||
idx(0) = l-1
|
||||
end
|
||||
|
||||
subroutine get_excitation_degree_vector_mono_or_exchange(key1,key2,degree,Nint,sze,idx)
|
||||
use bitmasks
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Applies get_excitation_degree to an array of determinants and return only the mono excitations
|
||||
! and the connections through exchange integrals
|
||||
END_DOC
|
||||
integer, intent(in) :: Nint, sze
|
||||
integer(bit_kind), intent(in) :: key1(Nint,2,sze)
|
||||
integer(bit_kind), intent(in) :: key2(Nint,2)
|
||||
integer, intent(out) :: degree(sze)
|
||||
integer, intent(out) :: idx(0:sze)
|
||||
|
||||
integer :: i,l,d,m
|
||||
integer :: exchange_1,exchange_2
|
||||
|
||||
ASSERT (Nint > 0)
|
||||
ASSERT (sze > 0)
|
||||
|
||||
l=1
|
||||
if (Nint==1) then
|
||||
|
||||
!DIR$ LOOP COUNT (1000)
|
||||
do i=1,sze
|
||||
d = popcnt(xor( key1(1,1,i), key2(1,1))) + &
|
||||
popcnt(xor( key1(1,2,i), key2(1,2)))
|
||||
exchange_1 = popcnt(xor(iand(key1(1,1,i),key1(1,2,i)),iand(key2(1,1),key2(1,2))))
|
||||
exchange_2 = popcnt(iand(xor(key1(1,1,i),key2(1,1)),xor(key1(1,2,i),key2(1,2))))
|
||||
if (d > 4)cycle
|
||||
if (d ==4)then
|
||||
if(exchange_1 .eq. 0 ) then
|
||||
degree(l) = ishft(d,-1)
|
||||
idx(l) = i
|
||||
l = l+1
|
||||
else if (exchange_1 .eq. 2 .and. exchange_2.eq.2)then
|
||||
degree(l) = ishft(d,-1)
|
||||
idx(l) = i
|
||||
l = l+1
|
||||
else
|
||||
cycle
|
||||
endif
|
||||
! pause
|
||||
else
|
||||
degree(l) = ishft(d,-1)
|
||||
idx(l) = i
|
||||
l = l+1
|
||||
endif
|
||||
enddo
|
||||
else if (Nint==2) then
|
||||
|
||||
!DIR$ LOOP COUNT (1000)
|
||||
do i=1,sze
|
||||
d = popcnt(xor( key1(1,1,i), key2(1,1))) + &
|
||||
popcnt(xor( key1(1,2,i), key2(1,2))) + &
|
||||
popcnt(xor( key1(2,1,i), key2(2,1))) + &
|
||||
popcnt(xor( key1(2,2,i), key2(2,2)))
|
||||
exchange_1 = popcnt(xor(iand(key1(1,1,i),key1(1,2,i)),iand(key2(1,2),key2(1,2)))) + &
|
||||
popcnt(xor(iand(key1(2,1,i),key1(2,2,i)),iand(key2(2,2),key2(2,2))))
|
||||
exchange_2 = popcnt(iand(xor(key1(1,1,i),key2(1,1)),xor(key1(1,2,i),key2(1,2)))) + &
|
||||
popcnt(iand(xor(key1(2,1,i),key2(2,1)),xor(key1(2,2,i),key2(2,2))))
|
||||
if (d > 4)cycle
|
||||
if (d ==4)then
|
||||
if(exchange_1 .eq. 0 ) then
|
||||
degree(l) = ishft(d,-1)
|
||||
idx(l) = i
|
||||
l = l+1
|
||||
else if (exchange_1 .eq. 2 .and. exchange_2.eq.2)then
|
||||
degree(l) = ishft(d,-1)
|
||||
idx(l) = i
|
||||
l = l+1
|
||||
else
|
||||
cycle
|
||||
endif
|
||||
! pause
|
||||
else
|
||||
degree(l) = ishft(d,-1)
|
||||
idx(l) = i
|
||||
l = l+1
|
||||
endif
|
||||
enddo
|
||||
|
||||
else if (Nint==3) then
|
||||
|
||||
!DIR$ LOOP COUNT (1000)
|
||||
do i=1,sze
|
||||
d = popcnt(xor( key1(1,1,i), key2(1,1))) + &
|
||||
popcnt(xor( key1(1,2,i), key2(1,2))) + &
|
||||
popcnt(xor( key1(2,1,i), key2(2,1))) + &
|
||||
popcnt(xor( key1(2,2,i), key2(2,2))) + &
|
||||
popcnt(xor( key1(3,1,i), key2(3,1))) + &
|
||||
popcnt(xor( key1(3,2,i), key2(3,2)))
|
||||
exchange_1 = popcnt(xor(iand(key1(1,1,i),key1(1,2,i)),iand(key2(1,1),key2(1,2)))) + &
|
||||
popcnt(xor(iand(key1(2,1,i),key1(2,2,i)),iand(key2(2,1),key2(2,2)))) + &
|
||||
popcnt(xor(iand(key1(3,1,i),key1(3,2,i)),iand(key2(3,1),key2(3,2))))
|
||||
exchange_2 = popcnt(iand(xor(key1(1,1,i),key2(1,1)),xor(key1(1,2,i),key2(1,2)))) + &
|
||||
popcnt(iand(xor(key1(2,1,i),key2(2,1)),xor(key1(2,2,i),key2(2,2)))) + &
|
||||
popcnt(iand(xor(key1(3,1,i),key2(3,1)),xor(key1(3,2,i),key2(3,2))))
|
||||
if (d > 4)cycle
|
||||
if (d ==4)then
|
||||
if(exchange_1 .eq. 0 ) then
|
||||
degree(l) = ishft(d,-1)
|
||||
idx(l) = i
|
||||
l = l+1
|
||||
else if (exchange_1 .eq. 2 .and. exchange_2.eq.2)then
|
||||
degree(l) = ishft(d,-1)
|
||||
idx(l) = i
|
||||
l = l+1
|
||||
else
|
||||
cycle
|
||||
endif
|
||||
! pause
|
||||
else
|
||||
degree(l) = ishft(d,-1)
|
||||
idx(l) = i
|
||||
l = l+1
|
||||
endif
|
||||
enddo
|
||||
|
||||
else
|
||||
|
||||
!DIR$ LOOP COUNT (1000)
|
||||
do i=1,sze
|
||||
d = 0
|
||||
exchange_1 = 0
|
||||
!DIR$ LOOP COUNT MIN(4)
|
||||
do m=1,Nint
|
||||
d = d + popcnt(xor( key1(m,1,i), key2(m,1))) &
|
||||
+ popcnt(xor( key1(m,2,i), key2(m,2)))
|
||||
exchange_1 = popcnt(xor(iand(key1(m,1,i),key1(m,2,i)),iand(key2(m,1),key2(m,2))))
|
||||
exchange_2 = popcnt(iand(xor(key1(m,1,i),key2(m,1)),xor(key1(m,2,i),key2(m,2))))
|
||||
enddo
|
||||
if (d > 4)cycle
|
||||
if (d ==4)then
|
||||
if(exchange_1 .eq. 0 ) then
|
||||
degree(l) = ishft(d,-1)
|
||||
idx(l) = i
|
||||
l = l+1
|
||||
else if (exchange_1 .eq. 2 .and. exchange_2.eq.2)then
|
||||
degree(l) = ishft(d,-1)
|
||||
idx(l) = i
|
||||
l = l+1
|
||||
else
|
||||
cycle
|
||||
endif
|
||||
! pause
|
||||
else
|
||||
degree(l) = ishft(d,-1)
|
||||
idx(l) = i
|
||||
l = l+1
|
||||
endif
|
||||
enddo
|
||||
|
||||
endif
|
||||
idx(0) = l-1
|
||||
end
|
||||
|
||||
|
||||
subroutine get_excitation_degree_vector(key1,key2,degree,Nint,sze,idx)
|
||||
use bitmasks
|
||||
|
|
Loading…
Reference in New Issue
Block a user