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139 lines
5.6 KiB
Fortran
139 lines
5.6 KiB
Fortran
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BEGIN_PROVIDER [double precision, two_e_int_hf_f, (n_basis_orb,n_basis_orb,n_max_occ_val_orb_for_hf,n_max_occ_val_orb_for_hf)]
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implicit none
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BEGIN_DOC
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! list of two-electron integrals (built with the MOs belonging to the \mathcal{B} space)
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!
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! needed to compute the function f_{HF}(r_1,r_2)
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!
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! two_e_int_hf_f(j,i,n,m) = < j i | n m > where all orbitals belong to "list_basis"
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END_DOC
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integer :: orb_i,orb_j,i,j,orb_m,orb_n,m,n
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double precision :: get_two_e_integral
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do orb_m = 1, n_max_occ_val_orb_for_hf! electron 1
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m = list_valence_orb_for_hf(orb_m,1)
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do orb_n = 1, n_max_occ_val_orb_for_hf! electron 2
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n = list_valence_orb_for_hf(orb_n,1)
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do orb_i = 1, n_basis_orb ! electron 1
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i = list_basis(orb_i)
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do orb_j = 1, n_basis_orb ! electron 2
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j = list_basis(orb_j)
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! 2 1 2 1
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two_e_int_hf_f(orb_j,orb_i,orb_n,orb_m) = get_two_e_integral(m,n,i,j,mo_integrals_map)
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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 f_HF_valence_ab(r1,r2,f_HF_val_ab,two_bod_dens)
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implicit none
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BEGIN_DOC
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! f_HF_val_ab(r1,r2) = function f_{\Psi^B}(X_1,X_2) of Eq. (22) of J. Chem. Phys. 149, 194301 (2018)
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!
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! for alpha beta spins and an HF wave function and excluding the "core" orbitals (see Eq. 16a of Phys.Chem.Lett.2019, 10, 2931 2937)
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!
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! two_bod_dens = on-top pair density of the HF wave function
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!
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! < HF | wee_{\alpha\beta} | HF > = \int (r1,r2) f_HF_ab(r1,r2) excluding all contributions from "core" "electrons"
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END_DOC
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double precision, intent(in) :: r1(3), r2(3)
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double precision, intent(out):: f_HF_val_ab,two_bod_dens
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integer :: i,j,m,n,i_m,i_n
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integer :: i_i,i_j
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double precision :: mo_two_e_integral
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double precision, allocatable :: mos_array_r1(:)
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double precision, allocatable :: mos_array_r2(:)
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double precision, allocatable :: mos_array_valence_r1(:),mos_array_valence_r2(:)
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double precision, allocatable :: mos_array_valence_hf_r1(:),mos_array_valence_hf_r2(:)
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double precision :: get_two_e_integral
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allocate(mos_array_valence_r1(n_basis_orb) , mos_array_valence_r2(n_basis_orb), mos_array_r1(mo_num), mos_array_r2(mo_num))
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allocate(mos_array_valence_hf_r1(n_occ_val_orb_for_hf(1)) , mos_array_valence_hf_r2(n_occ_val_orb_for_hf(2)) )
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! You get all orbitals in r_1 and r_2
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call give_all_mos_at_r(r1,mos_array_r1)
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call give_all_mos_at_r(r2,mos_array_r2)
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! You extract the occupied ALPHA/BETA orbitals belonging to the space \mathcal{A}
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do i_m = 1, n_occ_val_orb_for_hf(1)
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mos_array_valence_hf_r1(i_m) = mos_array_r1(list_valence_orb_for_hf(i_m,1))
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enddo
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do i_m = 1, n_occ_val_orb_for_hf(2)
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mos_array_valence_hf_r2(i_m) = mos_array_r2(list_valence_orb_for_hf(i_m,2))
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enddo
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! You extract the orbitals belonging to the space \mathcal{B}
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do i_m = 1, n_basis_orb
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mos_array_valence_r1(i_m) = mos_array_r1(list_basis(i_m))
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mos_array_valence_r2(i_m) = mos_array_r2(list_basis(i_m))
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enddo
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f_HF_val_ab = 0.d0
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two_bod_dens = 0.d0
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! You browse all OCCUPIED ALPHA electrons in the \mathcal{A} space
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do m = 1, n_occ_val_orb_for_hf(1)! electron 1
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! You browse all OCCUPIED BETA electrons in the \mathcal{A} space
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do n = 1, n_occ_val_orb_for_hf(2)! electron 2
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! two_bod_dens(r_1,r_2) = n_alpha(r_1) * n_beta(r_2)
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two_bod_dens += mos_array_valence_hf_r1(m) * mos_array_valence_hf_r1(m) * mos_array_valence_hf_r2(n) * mos_array_valence_hf_r2(n)
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! You browse all COUPLE OF ORBITALS in the \mathacal{B} space
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do i = 1, n_basis_orb
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do j = 1, n_basis_orb
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! 2 1 2 1
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f_HF_val_ab += two_e_int_hf_f(j,i,n,m) &
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* mos_array_valence_r1(i) * mos_array_valence_hf_r1(m) &
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* mos_array_valence_r2(j) * mos_array_valence_hf_r2(n)
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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 integral_f_HF_valence_ab(r1,int_f_HF_val_ab)
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implicit none
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BEGIN_DOC
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! in_f_HF_val_ab(r_1) = \int dr_2 f_{\Psi^B}(r_1,r_2)
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!
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! where f_{\Psi^B}(r_1,r_2) is defined by Eq. (22) of J. Chem. Phys. 149, 194301 (2018)
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!
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! for alpha beta spins and an HF wave function and excluding the "core" orbitals (see Eq. 16a of Phys.Chem.Lett.2019, 10, 2931 2937)
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!
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! Such function can be used to test if the f_HF_val_ab(r_1,r_2) is correctly built.
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!
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! < HF | wee_{\alpha\beta} | HF > = \int (r1) int_f_HF_val_ab(r_1)
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END_DOC
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double precision, intent(in) :: r1(3)
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double precision, intent(out):: int_f_HF_val_ab
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integer :: i,j,m,n,i_m,i_n
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integer :: i_i,i_j
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double precision :: mo_two_e_integral
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double precision :: mos_array_r1(mo_num)
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double precision, allocatable :: mos_array_valence_r1(:)
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double precision, allocatable :: mos_array_valence_hf_r1(:)
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double precision :: get_two_e_integral
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call give_all_mos_at_r(r1,mos_array_r1)
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allocate(mos_array_valence_r1( n_basis_orb ))
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allocate(mos_array_valence_hf_r1( n_occ_val_orb_for_hf(1) ) )
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do i_m = 1, n_occ_val_orb_for_hf(1)
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mos_array_valence_hf_r1(i_m) = mos_array_r1(list_valence_orb_for_hf(i_m,1))
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enddo
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do i_m = 1, n_basis_orb
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mos_array_valence_r1(i_m) = mos_array_r1(list_basis(i_m))
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enddo
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int_f_HF_val_ab = 0.d0
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! You browse all OCCUPIED ALPHA electrons in the \mathcal{A} space
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do m = 1, n_occ_val_orb_for_hf(1)! electron 1
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! You browse all OCCUPIED BETA electrons in the \mathcal{A} space
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do n = 1, n_occ_val_orb_for_hf(2)! electron 2
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! You browse all ORBITALS in the \mathacal{B} space
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do i = 1, n_basis_orb
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! due to integration in real-space and the use of orthonormal MOs, a Kronecker delta_jn shoes up
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j = n
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! 2 1 2 1
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int_f_HF_val_ab += two_e_int_hf_f(j,i,n,m) &
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* mos_array_valence_r1(i) * mos_array_valence_hf_r1(m)
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enddo
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enddo
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enddo
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end
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