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added two_body_dens_rout.irp.f
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Emmanuel Giner
parent
47c1bec1d8
commit
92ad3766eb
189
src/cas_based_on_top/two_body_dens_rout.irp.f
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189
src/cas_based_on_top/two_body_dens_rout.irp.f
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subroutine give_n2_ii_val_ab(r1,r2,two_bod_dens)
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implicit none
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BEGIN_DOC
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! contribution from purely inactive orbitals to n2_{\Psi^B}(r_1,r_2) for a CAS wave function
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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):: 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, allocatable :: mos_array_inact_r1(:),mos_array_inact_r2(:)
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double precision, allocatable :: mos_array_basis_r1(:),mos_array_basis_r2(:)
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double precision, allocatable :: mos_array_r1(:) , mos_array_r2(:)
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! You get all orbitals in r_1 and r_2
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allocate(mos_array_r1(mo_num) , mos_array_r2(mo_num) )
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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 inactive orbitals
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allocate(mos_array_inact_r1(n_inact_orb) , mos_array_inact_r2(n_inact_orb) )
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do i_m = 1, n_inact_orb
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mos_array_inact_r1(i_m) = mos_array_r1(list_inact(i_m))
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enddo
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do i_m = 1, n_inact_orb
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mos_array_inact_r2(i_m) = mos_array_r2(list_inact(i_m))
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enddo
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! You extract the orbitals belonging to the space \mathcal{B}
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allocate(mos_array_basis_r1(n_basis_orb) , mos_array_basis_r2(n_basis_orb) )
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do i_m = 1, n_basis_orb
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mos_array_basis_r1(i_m) = mos_array_r1(list_basis(i_m))
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mos_array_basis_r2(i_m) = mos_array_r2(list_basis(i_m))
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enddo
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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_inact_orb ! 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_inact_orb ! 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_inact_r1(m) * mos_array_inact_r1(m) * mos_array_inact_r2(n) * mos_array_inact_r2(n)
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enddo
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enddo
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end
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subroutine give_n2_ia_val_ab(r1,r2,two_bod_dens,istate)
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BEGIN_DOC
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! contribution from inactive and active orbitals to n2_{\Psi^B}(r_1,r_2) for the "istate" state of a CAS wave function
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END_DOC
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implicit none
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integer, intent(in) :: istate
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double precision, intent(in) :: r1(3),r2(3)
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double precision, intent(out):: two_bod_dens
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integer :: i,orb_i,a,orb_a,n,m,b
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double precision :: rho
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double precision, allocatable :: mos_array_r1(:) , mos_array_r2(:)
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double precision, allocatable :: mos_array_inact_r1(:),mos_array_inact_r2(:)
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double precision, allocatable :: mos_array_basis_r1(:),mos_array_basis_r2(:)
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double precision, allocatable :: mos_array_act_r1(:),mos_array_act_r2(:)
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two_bod_dens = 0.d0
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! You get all orbitals in r_1 and r_2
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allocate(mos_array_r1(mo_num) , mos_array_r2(mo_num) )
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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 inactive orbitals
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allocate( mos_array_inact_r1(n_inact_orb) , mos_array_inact_r2(n_inact_orb) )
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do i = 1, n_inact_orb
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mos_array_inact_r1(i) = mos_array_r1(list_inact(i))
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enddo
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do i= 1, n_inact_orb
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mos_array_inact_r2(i) = mos_array_r2(list_inact(i))
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enddo
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! You extract the active orbitals
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allocate( mos_array_act_r1(n_basis_orb) , mos_array_act_r2(n_basis_orb) )
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do i= 1, n_act_orb
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mos_array_act_r1(i) = mos_array_r1(list_act(i))
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enddo
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do i= 1, n_act_orb
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mos_array_act_r2(i) = mos_array_r2(list_act(i))
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enddo
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! You extract the orbitals belonging to the space \mathcal{B}
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allocate( mos_array_basis_r1(n_basis_orb) , mos_array_basis_r2(n_basis_orb) )
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do i= 1, n_basis_orb
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mos_array_basis_r1(i) = mos_array_r1(list_basis(i))
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enddo
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do i= 1, n_basis_orb
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mos_array_basis_r2(i) = mos_array_r2(list_basis(i))
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enddo
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! Contracted density : intermediate quantity
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! rho_tilde(i,a) = \sum_b rho(b,a) * phi_i(1) * phi_j(2)
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allocate(rho_tilde(n_inact_orb,n_act_orb))
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two_bod_dens = 0.d0
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do a = 1, n_act_orb
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do i = 1, n_inact_orb
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rho_tilde(i,a) = 0.d0
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do b = 1, n_act_orb
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rho = one_e_act_dm_beta_mo_for_dft(b,a,istate) + one_e_act_dm_alpha_mo_for_dft(b,a,istate)
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two_bod_dens += mos_array_inact_r1(i) * mos_array_inact_r1(i) * mos_array_act_r2(a) * mos_array_act_r2(b) * rho
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rho_tilde(i,a) += rho * mos_array_inact_r1(i) * mos_array_act_r2(b)
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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_n2_aa_val_ab(r1,r2,two_bod_dens,istate)
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BEGIN_DOC
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! contribution from purely active orbitals to n2_{\Psi^B}(r_1,r_2) for the "istate" state of a CAS wave function
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END_DOC
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implicit none
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integer, intent(in) :: istate
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double precision, intent(in) :: r1(3),r2(3)
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double precision, intent(out):: two_bod_dens
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integer :: i,orb_i,a,orb_a,n,m,b,c,d
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double precision :: rho
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double precision, allocatable :: mos_array_r1(:) , mos_array_r2(:)
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double precision, allocatable :: mos_array_basis_r1(:),mos_array_basis_r2(:)
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double precision, allocatable :: mos_array_act_r1(:),mos_array_act_r2(:)
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two_bod_dens = 0.d0
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! You get all orbitals in r_1 and r_2
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allocate(mos_array_r1(mo_num) , mos_array_r2(mo_num) )
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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 active orbitals
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allocate( mos_array_act_r1(n_basis_orb) , mos_array_act_r2(n_basis_orb) )
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do i= 1, n_act_orb
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mos_array_act_r1(i) = mos_array_r1(list_act(i))
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enddo
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do i= 1, n_act_orb
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mos_array_act_r2(i) = mos_array_r2(list_act(i))
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enddo
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! You extract the orbitals belonging to the space \mathcal{B}
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allocate( mos_array_basis_r1(n_basis_orb) , mos_array_basis_r2(n_basis_orb) )
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do i= 1, n_basis_orb
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mos_array_basis_r1(i) = mos_array_r1(list_basis(i))
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enddo
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do i= 1, n_basis_orb
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mos_array_basis_r2(i) = mos_array_r2(list_basis(i))
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enddo
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! Contracted density : intermediate quantity
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! rho_tilde(i,a) = \sum_b rho(b,a) * phi_i(1) * phi_j(2)
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allocate(rho_tilde(n_act_orb,n_act_orb))
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two_bod_dens = 0.d0
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rho_tilde = 0.d0
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do a = 1, n_act_orb ! 1
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do b = 1, n_act_orb ! 2
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do c = 1, n_act_orb ! 1
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do d = 1, n_act_orb ! 2
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rho = mos_array_act_r1(c) * mos_array_act_r2(d) * act_2_rdm_ab_mo(d,c,b,a,istate)
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rho_tilde(b,a) += rho
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two_bod_dens += rho * mos_array_act_r1(a) * mos_array_act_r2(b)
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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_n2_cas(r1,r2,istate,n2_psi)
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implicit none
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BEGIN_DOC
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! returns mu(r), f_psi, n2_psi for a general cas wave function
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END_DOC
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integer, intent(in) :: istate
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double precision, intent(in) :: r1(3),r2(3)
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double precision, intent(out) :: n2_psi
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double precision :: two_bod_dens_ii
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double precision :: two_bod_dens_ia
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double precision :: two_bod_dens_aa
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! inactive-inactive part of n2_psi(r1,r2)
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call give_n2_ii_val_ab(r,r,two_bod_dens_ii)
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! inactive-active part of n2_psi(r1,r2)
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call give_n2_ia_val_ab(r,r,two_bod_dens_ia,istate)
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! active-active part of n2_psi(r1,r2)
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call give_n2_aa_val_ab(r,r,two_bod_dens_aa,istate)
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n2_psi = n2_ii_val_ab + n2_ia_val_ab + n2_aa_val_ab
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n2_psi = two_bod_dens_ii + two_bod_dens_ia + two_bod_dens_aa
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end
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@ -2,6 +2,8 @@
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BEGIN_PROVIDER [double precision, act_2_rdm_ab_mo, (n_act_orb,n_act_orb,n_act_orb,n_act_orb,N_states)]
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implicit none
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BEGIN_DOC
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! 12 12
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! 1 2 1 2 == <ij|kl>
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! act_2_rdm_ab_mo(i,j,k,l,istate) = STATE SPECIFIC physicist notation for 2RDM of alpha/beta electrons
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!
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! <Psi_{istate}| a^{\dagger}_{i \alpha} a^{\dagger}_{j \beta} a_{l \beta} a_{k \alpha} |Psi_{istate}>
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