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QuantumPackage/plugins/local/tc_bi_ortho/slater_tc_opt.irp.f

173 lines
4.3 KiB
Fortran

! ---
subroutine provide_all_three_ints_bi_ortho()
BEGIN_DOC
! routine that provides all necessary three-electron integrals
END_DOC
implicit none
PROVIDE ao_two_e_integrals_in_map
if(three_body_h_tc) then
if(three_e_3_idx_term) then
PROVIDE three_e_3_idx_direct_bi_ort three_e_3_idx_cycle_1_bi_ort three_e_3_idx_cycle_2_bi_ort
PROVIDE three_e_3_idx_exch23_bi_ort three_e_3_idx_exch13_bi_ort three_e_3_idx_exch12_bi_ort
endif
if(three_e_4_idx_term) then
PROVIDE three_e_4_idx_direct_bi_ort three_e_4_idx_cycle_1_bi_ort three_e_4_idx_exch23_bi_ort three_e_4_idx_exch13_bi_ort
endif
if(pure_three_body_h_tc)then
provide three_body_ints_bi_ort
endif
if(.not. double_normal_ord .and. three_e_5_idx_term) then
PROVIDE three_e_5_idx_direct_bi_ort
elseif(double_normal_ord .and. (.not. three_e_5_idx_term)) then
PROVIDE normal_two_body_bi_orth
endif
endif
return
end
! ---
subroutine htilde_mu_mat_opt_bi_ortho_tot(key_j, key_i, Nint, htot)
implicit none
BEGIN_DOC
!
! <key_j |H_tilde | key_i> where |key_j> is developed on the LEFT basis and |key_i> is developed on the RIGHT basis
!!
! Returns the total matrix element
!! WARNING !!
!
! Non hermitian !!
!
END_DOC
use bitmasks
integer, intent(in) :: Nint
integer(bit_kind), intent(in) :: key_i(Nint,2), key_j(Nint,2)
double precision, intent(out) :: htot
double precision :: hmono, htwoe, hthree
call htilde_mu_mat_opt_bi_ortho(key_j, key_i, Nint, hmono, htwoe, hthree, htot)
end
! ---
subroutine htilde_mu_mat_opt_bi_ortho(key_j, key_i, Nint, hmono, htwoe, hthree, htot)
BEGIN_DOC
!
! <key_j |H_tilde | key_i> where |key_j> is developed on the LEFT basis and |key_i> is developed on the RIGHT basis
!!
! Returns the detail of the matrix element in terms of single, two and three electron contribution.
!! WARNING !!
!
! Non hermitian !!
!
END_DOC
use bitmasks
implicit none
integer, intent(in) :: Nint
integer(bit_kind), intent(in) :: key_i(Nint,2), key_j(Nint,2)
double precision, intent(out) :: hmono, htwoe, hthree, htot
integer :: degree
hmono = 0.d0
htwoe = 0.d0
htot = 0.d0
hthree = 0.d0
call get_excitation_degree(key_i, key_j, degree, Nint)
if(.not.pure_three_body_h_tc) then
if(degree .gt. 2) return
if(degree == 0) then
call diag_htilde_mu_mat_fock_bi_ortho (Nint, key_i, hmono, htwoe, hthree, htot)
else if (degree == 1) then
call single_htilde_mu_mat_fock_bi_ortho(Nint, key_j, key_i , hmono, htwoe, hthree, htot)
else if(degree == 2) then
call double_htilde_mu_mat_fock_bi_ortho(Nint, key_j, key_i, hmono, htwoe, hthree, htot)
endif
else
if(degree .gt. 3) return
if(degree == 0) then
call diag_htilde_mu_mat_fock_bi_ortho (Nint, key_i, hmono, htwoe, hthree, htot)
else if (degree == 1) then
call single_htilde_mu_mat_fock_bi_ortho(Nint, key_j, key_i , hmono, htwoe, hthree, htot)
else if(degree == 2) then
call double_htilde_mu_mat_fock_bi_ortho(Nint, key_j, key_i, hmono, htwoe, hthree, htot)
else
call triple_htilde_mu_mat_fock_bi_ortho(Nint, key_j, key_i, hmono, htwoe, hthree, htot)
endif
endif
if(degree==0) then
htot += nuclear_repulsion
endif
end
! ---
subroutine htilde_mu_mat_opt_bi_ortho_no_3e(key_j, key_i, Nint, htot)
BEGIN_DOC
!
! <key_j |H_tilde | key_i> where |key_j> is developed on the LEFT basis and |key_i> is developed on the RIGHT basis
!!
! Returns the detail of the matrix element WITHOUT ANY CONTRIBUTION FROM THE THREE ELECTRON TERMS
!! WARNING !!
!
! Non hermitian !!
!
END_DOC
use bitmasks
implicit none
integer, intent(in) :: Nint
integer(bit_kind), intent(in) :: key_i(Nint,2), key_j(Nint,2)
double precision, intent(out) :: htot
integer :: degree
htot = 0.d0
call get_excitation_degree(key_i, key_j, degree, Nint)
if(degree.gt.2) return
if(degree == 0)then
call diag_htilde_mu_mat_fock_bi_ortho_no_3e(Nint, key_i,htot)
else if (degree == 1)then
call single_htilde_mu_mat_fock_bi_ortho_no_3e(Nint,key_j, key_i , htot)
else if(degree == 2)then
call double_htilde_mu_mat_fock_bi_ortho_no_3e(Nint, key_j, key_i, htot)
endif
if(degree==0) then
htot += nuclear_repulsion
endif
end
! ---