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beginning to optimize the double excitations for TC
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@ -7,7 +7,7 @@ BEGIN_PROVIDER [ double precision, three_e_5_idx_direct_bi_ort, (mo_num, mo_num,
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!
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! matrix element of the -L three-body operator FOR THE DIRECT TERMS OF DOUBLE EXCITATIONS AND BI ORTHO MOs
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!
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! three_e_5_idx_direct_bi_ort(m,l,j,k,i) = <mjk|-L|mji> ::: notice that i is the RIGHT MO and k is the LEFT MO
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! three_e_5_idx_direct_bi_ort(m,l,j,k,i) = <mlk|-L|mji> ::: notice that i is the RIGHT MO and k is the LEFT MO
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!
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! notice the -1 sign: in this way three_e_3_idx_direct_bi_ort can be directly used to compute Slater rules with a + sign
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END_DOC
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@ -202,7 +202,7 @@ BEGIN_PROVIDER [ double precision, three_e_5_idx_exch13_bi_ort, (mo_num, mo_num,
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!
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! matrix element of the -L three-body operator FOR THE DIRECT TERMS OF DOUBLE EXCITATIONS AND BI ORTHO MOs
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!
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! three_e_5_idx_exch13_bi_ort(m,l,j,k,i) = <mlk|-L|jmi> ::: notice that i is the RIGHT MO and k is the LEFT MO
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! three_e_5_idx_exch13_bi_ort(m,l,j,k,i) = <mlk|-L|ijm> ::: notice that i is the RIGHT MO and k is the LEFT MO
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!
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! notice the -1 sign: in this way three_e_3_idx_direct_bi_ort can be directly used to compute Slater rules with a + sign
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!
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@ -251,7 +251,7 @@ BEGIN_PROVIDER [ double precision, three_e_5_idx_exch12_bi_ort, (mo_num, mo_num,
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!
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! matrix element of the -L three-body operator FOR THE DIRECT TERMS OF DOUBLE EXCITATIONS AND BI ORTHO MOs
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!
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! three_e_5_idx_exch12_bi_ort(m,l,j,k,i) = <mlk|-L|jmi> ::: notice that i is the RIGHT MO and k is the LEFT MO
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! three_e_5_idx_exch12_bi_ort(m,l,j,k,i) = <mlk|-L|mij> ::: notice that i is the RIGHT MO and k is the LEFT MO
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!
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! notice the -1 sign: in this way three_e_3_idx_direct_bi_ort can be directly used to compute Slater rules with a + sign
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!
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57
src/tc_bi_ortho/slater_tc_opt_double.irp.f
Normal file
57
src/tc_bi_ortho/slater_tc_opt_double.irp.f
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@ -0,0 +1,57 @@
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BEGIN_PROVIDER [ double precision, eff_2_e_from_3_e_ab, (mo_num, mo_num, mo_num, mo_num)]
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implicit none
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BEGIN_DOC
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! eff_2_e_from_3_e_ab(p2,p1,h2,h1) = Effective Two-electron operator for alpha/beta double excitations
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!
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! from contraction with HF density = a^{dagger}_p1_alpha a^{dagger}_p2_beta a_h2_beta a_h1_alpha
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END_DOC
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integer :: i,h1,p1,h2,p2
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integer :: hh1,hh2,pp1,pp2,m,mm
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integer :: Ne(2)
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integer, allocatable :: occ(:,:)
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double precision :: contrib
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allocate( occ(N_int*bit_kind_size,2) )
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call bitstring_to_list_ab(ref_bitmask,occ,Ne,N_int)
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eff_2_e_from_3_e_ab = 0.d0
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do hh1 = 1, n_act_orb !! alpha
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h1 = list_act(hh1)
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do hh2 = 1, n_act_orb !! beta
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h2 = list_act(hh2)
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do pp1 = 1, n_act_orb !! alpha
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p1 = list_act(pp1)
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do pp2 = 1, n_act_orb !! beta
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p2 = list_act(pp2)
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call give_contrib_for_abab(h1,h2,p1,p2,occ,Ne,contrib)
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eff_2_e_from_3_e_ab(p2,p1,h2,h1) = contrib
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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_PROVIDER
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subroutine give_contrib_for_abab(h1,h2,p1,p2,occ,Ne,contrib)
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implicit none
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integer, intent(in) :: h1,h2,p1,p2,occ(N_int*bit_kind_size,2),Ne(2)
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double precision, intent(out) :: contrib
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integer :: mm,m
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double precision :: direct_int, exchange_int
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!! h1,p1 == alpha
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!! h2,p2 == beta
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contrib = 0.d0
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do mm = 1, Ne(1) !! alpha
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m = occ(m,1)
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direct_int = three_e_5_idx_direct_bi_ort(mm,p2,h2,p1,h1)
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! exchange between (h1,p1) and m
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exchange_int = three_e_5_idx_exch13_bi_ort(mm,p2,h2,p1,h1)
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contrib += direct_int - exchange_int
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enddo
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do mm = 1, Ne(2) !! beta
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m = occ(m,2)
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direct_int = three_e_5_idx_direct_bi_ort(mm,p2,h2,p1,h1)
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! exchange between (h2,p2) and m
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exchange_int = three_e_5_idx_exch23_bi_ort(mm,p2,h2,p1,h1)
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contrib += direct_int - exchange_int
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enddo
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end
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@ -10,6 +10,7 @@ program test_normal_order
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read_wf = .True.
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touch read_wf
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touch my_grid_becke my_n_pt_r_grid my_n_pt_a_grid
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call provide_all_three_ints_bi_ortho
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call test
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end
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@ -28,7 +29,7 @@ subroutine test
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s2 = 2
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accu = 0.d0
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do h1 = 1, elec_beta_num
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do p1 = elec_beta_num+1, mo_num
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do p1 = elec_alpha_num+1, mo_num
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do h2 = 1, elec_beta_num
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do p2 = elec_beta_num+1, mo_num
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det_i = ref_bitmask
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@ -38,36 +39,37 @@ subroutine test
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call get_excitation_degree(ref_bitmask,det_i,degree,N_int)
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call get_excitation(ref_bitmask,det_i,exc,degree,phase,N_int)
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hthree *= phase
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normal = normal_two_body_bi_orth_ab(p2,h2,p1,h1)
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! normal = normal_two_body_bi_orth_ab(p2,h2,p1,h1)
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normal = eff_2_e_from_3_e_ab(p2,p1,h2,h1)
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accu += dabs(hthree-normal)
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enddo
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enddo
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enddo
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enddo
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print*,'accu opposite spin = ',accu
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print*,'accu opposite spin = ',accu
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s1 = 2
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s2 = 2
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accu = 0.d0
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do h1 = 1, elec_beta_num
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do p1 = elec_beta_num+1, mo_num
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do h2 = h1+1, elec_beta_num
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do p2 = elec_beta_num+1, mo_num
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det_i = ref_bitmask
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call do_single_excitation(det_i,h1,p1,s1,i_ok)
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call do_single_excitation(det_i,h2,p2,s2,i_ok)
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if(i_ok.ne.1)cycle
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call htilde_mu_mat_bi_ortho(det_i,ref_bitmask,N_int,hmono,htwoe,hthree,htilde_ij)
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call get_excitation_degree(ref_bitmask,det_i,degree,N_int)
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call get_excitation(ref_bitmask,det_i,exc,degree,phase,N_int)
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hthree *= phase
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normal = normal_two_body_bi_orth_aa_bb(p2,h2,p1,h1)
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accu += dabs(hthree-normal)
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enddo
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enddo
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enddo
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enddo
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print*,'accu same spin = ',accu
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!s1 = 2
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!s2 = 2
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!accu = 0.d0
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!do h1 = 1, elec_beta_num
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! do p1 = elec_beta_num+1, mo_num
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! do h2 = h1+1, elec_beta_num
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! do p2 = elec_beta_num+1, mo_num
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! det_i = ref_bitmask
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! call do_single_excitation(det_i,h1,p1,s1,i_ok)
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! call do_single_excitation(det_i,h2,p2,s2,i_ok)
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! if(i_ok.ne.1)cycle
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! call htilde_mu_mat_bi_ortho(det_i,ref_bitmask,N_int,hmono,htwoe,hthree,htilde_ij)
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! call get_excitation_degree(ref_bitmask,det_i,degree,N_int)
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! call get_excitation(ref_bitmask,det_i,exc,degree,phase,N_int)
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! hthree *= phase
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! normal = normal_two_body_bi_orth_aa_bb(p2,h2,p1,h1)
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! accu += dabs(hthree-normal)
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! enddo
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! enddo
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! enddo
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!enddo
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!print*,'accu same spin = ',accu
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end
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