mirror of
https://github.com/QuantumPackage/qp2.git
synced 2024-11-08 06:23:37 +01:00
364 lines
11 KiB
Fortran
364 lines
11 KiB
Fortran
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subroutine i_Wee_j_mono(key_i,key_j,Nint,spin,hij)
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use bitmasks
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implicit none
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BEGIN_DOC
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! Returns $\langle i|H|j \rangle$ where $i$ and $j$ are determinants differing by a
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! single excitation.
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END_DOC
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integer, intent(in) :: Nint, spin
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integer(bit_kind), intent(in) :: key_i(Nint,2), key_j(Nint,2)
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double precision, intent(out) :: hij
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integer :: exc(0:2,2)
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double precision :: phase
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PROVIDE big_array_exchange_integrals mo_two_e_integrals_in_map
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call get_mono_excitation_spin(key_i(1,spin),key_j(1,spin),exc,phase,Nint)
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call mono_excitation_wee(key_i,key_j,exc(1,1),exc(1,2),spin,phase,hij)
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end
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double precision function diag_wee_mat_elem(det_in,Nint)
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implicit none
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BEGIN_DOC
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! Computes $\langle i|H|i \rangle$.
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END_DOC
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integer,intent(in) :: Nint
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integer(bit_kind),intent(in) :: det_in(Nint,2)
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integer(bit_kind) :: hole(Nint,2)
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integer(bit_kind) :: particle(Nint,2)
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integer :: i, nexc(2), ispin
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integer :: occ_particle(Nint*bit_kind_size,2)
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integer :: occ_hole(Nint*bit_kind_size,2)
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integer(bit_kind) :: det_tmp(Nint,2)
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integer :: na, nb
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ASSERT (Nint > 0)
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ASSERT (sum(popcnt(det_in(:,1))) == elec_alpha_num)
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ASSERT (sum(popcnt(det_in(:,2))) == elec_beta_num)
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nexc(1) = 0
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nexc(2) = 0
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do i=1,Nint
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hole(i,1) = xor(det_in(i,1),ref_bitmask(i,1))
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hole(i,2) = xor(det_in(i,2),ref_bitmask(i,2))
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particle(i,1) = iand(hole(i,1),det_in(i,1))
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particle(i,2) = iand(hole(i,2),det_in(i,2))
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hole(i,1) = iand(hole(i,1),ref_bitmask(i,1))
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hole(i,2) = iand(hole(i,2),ref_bitmask(i,2))
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nexc(1) = nexc(1) + popcnt(hole(i,1))
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nexc(2) = nexc(2) + popcnt(hole(i,2))
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enddo
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diag_wee_mat_elem = ref_bitmask_two_e_energy
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if (nexc(1)+nexc(2) == 0) then
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return
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endif
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!call debug_det(det_in,Nint)
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integer :: tmp(2)
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!DIR$ FORCEINLINE
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call bitstring_to_list_ab(particle, occ_particle, tmp, Nint)
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ASSERT (tmp(1) == nexc(1))
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ASSERT (tmp(2) == nexc(2))
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!DIR$ FORCEINLINE
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call bitstring_to_list_ab(hole, occ_hole, tmp, Nint)
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ASSERT (tmp(1) == nexc(1))
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ASSERT (tmp(2) == nexc(2))
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det_tmp = ref_bitmask
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do ispin=1,2
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na = elec_num_tab(ispin)
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nb = elec_num_tab(iand(ispin,1)+1)
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do i=1,nexc(ispin)
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!DIR$ FORCEINLINE
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call ac_operator_two_e( occ_particle(i,ispin), ispin, det_tmp, diag_wee_mat_elem, Nint,na,nb)
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!DIR$ FORCEINLINE
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call a_operator_two_e ( occ_hole (i,ispin), ispin, det_tmp, diag_wee_mat_elem, Nint,na,nb)
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enddo
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enddo
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end
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subroutine a_operator_two_e(iorb,ispin,key,hjj,Nint,na,nb)
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use bitmasks
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implicit none
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BEGIN_DOC
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! Needed for :c:func:`diag_Wee_mat_elem`.
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END_DOC
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integer, intent(in) :: iorb, ispin, Nint
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integer, intent(inout) :: na, nb
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integer(bit_kind), intent(inout) :: key(Nint,2)
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double precision, intent(inout) :: hjj
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integer :: occ(Nint*bit_kind_size,2)
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integer :: other_spin
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integer :: k,l,i
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integer :: tmp(2)
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ASSERT (iorb > 0)
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ASSERT (ispin > 0)
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ASSERT (ispin < 3)
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ASSERT (Nint > 0)
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k = ishft(iorb-1,-bit_kind_shift)+1
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ASSERT (k > 0)
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l = iorb - ishft(k-1,bit_kind_shift)-1
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key(k,ispin) = ibclr(key(k,ispin),l)
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other_spin = iand(ispin,1)+1
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!DIR$ FORCEINLINE
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call bitstring_to_list_ab(key, occ, tmp, Nint)
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na = na-1
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! Same spin
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do i=1,na
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hjj = hjj - mo_two_e_integrals_jj_anti(occ(i,ispin),iorb)
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enddo
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! Opposite spin
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do i=1,nb
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hjj = hjj - mo_two_e_integrals_jj(occ(i,other_spin),iorb)
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enddo
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end
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subroutine ac_operator_two_e(iorb,ispin,key,hjj,Nint,na,nb)
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use bitmasks
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implicit none
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BEGIN_DOC
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! Needed for :c:func:`diag_Wee_mat_elem`.
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END_DOC
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integer, intent(in) :: iorb, ispin, Nint
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integer, intent(inout) :: na, nb
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integer(bit_kind), intent(inout) :: key(Nint,2)
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double precision, intent(inout) :: hjj
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integer :: occ(Nint*bit_kind_size,2)
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integer :: other_spin
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integer :: k,l,i
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ASSERT (iorb > 0)
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ASSERT (ispin > 0)
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ASSERT (ispin < 3)
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ASSERT (Nint > 0)
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integer :: tmp(2)
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!DIR$ FORCEINLINE
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call bitstring_to_list_ab(key, occ, tmp, Nint)
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ASSERT (tmp(1) == elec_alpha_num)
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ASSERT (tmp(2) == elec_beta_num)
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k = ishft(iorb-1,-bit_kind_shift)+1
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ASSERT (k > 0)
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l = iorb - ishft(k-1,bit_kind_shift)-1
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key(k,ispin) = ibset(key(k,ispin),l)
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other_spin = iand(ispin,1)+1
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! Same spin
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do i=1,na
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hjj = hjj + mo_two_e_integrals_jj_anti(occ(i,ispin),iorb)
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enddo
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! Opposite spin
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do i=1,nb
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hjj = hjj + mo_two_e_integrals_jj(occ(i,other_spin),iorb)
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enddo
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na = na+1
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end
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subroutine i_H_j_mono_spin_one_e(key_i,key_j,Nint,spin,hij)
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use bitmasks
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implicit none
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BEGIN_DOC
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! Returns $\langle i|H|j \rangle$ where $i$ and $j$ are determinants differing by
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! a single excitation.
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END_DOC
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integer, intent(in) :: Nint, spin
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integer(bit_kind), intent(in) :: key_i(Nint,2), key_j(Nint,2)
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double precision, intent(out) :: hij
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integer :: exc(0:2,2)
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double precision :: phase
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call get_mono_excitation_spin(key_i(1,spin),key_j(1,spin),exc,phase,Nint)
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integer :: m,p
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m = exc(1,1)
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p = exc(1,2)
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hij = phase * mo_one_e_integrals(m,p)
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end
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double precision function diag_H_mat_elem_one_e(det_in,Nint)
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use bitmasks
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implicit none
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BEGIN_DOC
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! Computes $\langle i|H|i \rangle$.
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END_DOC
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integer,intent(in) :: Nint
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integer(bit_kind),intent(in) :: det_in(Nint,2)
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integer(bit_kind) :: hole(Nint,2)
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integer(bit_kind) :: particle(Nint,2)
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integer :: i, nexc(2), ispin
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integer :: occ_particle(Nint*bit_kind_size,2)
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integer :: occ_hole(Nint*bit_kind_size,2)
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integer(bit_kind) :: det_tmp(Nint,2)
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integer :: na, nb
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ASSERT (Nint > 0)
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ASSERT (sum(popcnt(det_in(:,1))) == elec_alpha_num)
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ASSERT (sum(popcnt(det_in(:,2))) == elec_beta_num)
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diag_H_mat_elem_one_e = 0.d0
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!call debug_det(det_in,Nint)
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integer :: tmp(2)
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!DIR$ FORCEINLINE
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call bitstring_to_list_ab(det_in, occ_particle, tmp, Nint)
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do ispin = 1,2
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do i = 1, tmp(ispin)
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diag_H_mat_elem_one_e += mo_one_e_integrals(occ_particle(i,ispin),occ_particle(i,ispin))
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enddo
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enddo
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end
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subroutine i_H_j_one_e(key_i,key_j,Nint,hij)
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use bitmasks
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implicit none
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BEGIN_DOC
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! Returns $\langle i|H|j \rangle$ where $i$ and $j$ are determinants.
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END_DOC
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integer, intent(in) :: Nint
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integer(bit_kind), intent(in) :: key_i(Nint,2), key_j(Nint,2)
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double precision, intent(out) :: hij
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integer :: degree,m,p
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double precision :: diag_H_mat_elem_one_e,phase
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integer :: exc(0:2,2,2)
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call get_excitation_degree(key_i,key_j,degree,Nint)
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hij = 0.d0
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if(degree>1)then
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return
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endif
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if(degree==0)then
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hij = diag_H_mat_elem_one_e(key_i,N_int)
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else
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call get_mono_excitation(key_i,key_j,exc,phase,Nint)
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if (exc(0,1,1) == 1) then
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! Mono alpha
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m = exc(1,1,1)
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p = exc(1,2,1)
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else
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! Mono beta
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m = exc(1,1,2)
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p = exc(1,2,2)
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endif
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hij = phase * mo_one_e_integrals(m,p)
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endif
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end
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subroutine i_H_j_two_e(key_i,key_j,Nint,hij)
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use bitmasks
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implicit none
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BEGIN_DOC
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! Returns $\langle i|H|j \rangle$ where $i$ and $j$ are determinants.
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END_DOC
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integer, intent(in) :: Nint
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integer(bit_kind), intent(in) :: key_i(Nint,2), key_j(Nint,2)
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double precision, intent(out) :: hij
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integer :: exc(0:2,2,2)
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integer :: degree
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double precision :: get_two_e_integral
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integer :: m,n,p,q
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integer :: i,j,k
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integer :: occ(Nint*bit_kind_size,2)
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double precision :: diag_H_mat_elem, phase,phase_2
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integer :: n_occ_ab(2)
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PROVIDE mo_two_e_integrals_in_map mo_integrals_map big_array_exchange_integrals ref_bitmask_two_e_energy
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ASSERT (Nint > 0)
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ASSERT (Nint == N_int)
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ASSERT (sum(popcnt(key_i(:,1))) == elec_alpha_num)
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ASSERT (sum(popcnt(key_i(:,2))) == elec_beta_num)
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ASSERT (sum(popcnt(key_j(:,1))) == elec_alpha_num)
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ASSERT (sum(popcnt(key_j(:,2))) == elec_beta_num)
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hij = 0.d0
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!DIR$ FORCEINLINE
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call get_excitation_degree(key_i,key_j,degree,Nint)
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integer :: spin
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select case (degree)
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case (2)
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call get_double_excitation(key_i,key_j,exc,phase,Nint)
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if (exc(0,1,1) == 1) then
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! Mono alpha, mono beta
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if(exc(1,1,1) == exc(1,2,2) )then
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hij = phase * big_array_exchange_integrals(exc(1,1,1),exc(1,1,2),exc(1,2,1))
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else if (exc(1,2,1) ==exc(1,1,2))then
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hij = phase * big_array_exchange_integrals(exc(1,2,1),exc(1,1,1),exc(1,2,2))
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else
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hij = phase*get_two_e_integral( &
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exc(1,1,1), &
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exc(1,1,2), &
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exc(1,2,1), &
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exc(1,2,2) ,mo_integrals_map)
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endif
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else if (exc(0,1,1) == 2) then
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! Double alpha
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hij = phase*(get_two_e_integral( &
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exc(1,1,1), &
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exc(2,1,1), &
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exc(1,2,1), &
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exc(2,2,1) ,mo_integrals_map) - &
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get_two_e_integral( &
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exc(1,1,1), &
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exc(2,1,1), &
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exc(2,2,1), &
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exc(1,2,1) ,mo_integrals_map) )
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else if (exc(0,1,2) == 2) then
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! Double beta
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hij = phase*(get_two_e_integral( &
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exc(1,1,2), &
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exc(2,1,2), &
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exc(1,2,2), &
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exc(2,2,2) ,mo_integrals_map) - &
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get_two_e_integral( &
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exc(1,1,2), &
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exc(2,1,2), &
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exc(2,2,2), &
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exc(1,2,2) ,mo_integrals_map) )
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|
|
endif
|
||
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case (1)
|
||
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call get_mono_excitation(key_i,key_j,exc,phase,Nint)
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!DIR$ FORCEINLINE
|
||
|
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call bitstring_to_list_ab(key_i, occ, n_occ_ab, Nint)
|
||
|
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if (exc(0,1,1) == 1) then
|
||
|
|
! Mono alpha
|
||
|
|
m = exc(1,1,1)
|
||
|
|
p = exc(1,2,1)
|
||
|
|
spin = 1
|
||
|
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else
|
||
|
|
! Mono beta
|
||
|
|
m = exc(1,1,2)
|
||
|
|
p = exc(1,2,2)
|
||
|
|
spin = 2
|
||
|
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endif
|
||
|
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call mono_excitation_wee(key_i,key_j,p,m,spin,phase,hij)
|
||
|
|
case (0)
|
||
|
|
double precision :: diag_wee_mat_elem
|
||
|
|
hij = diag_wee_mat_elem(key_i,Nint)
|
||
|
|
end select
|
||
|
|
end
|
||
|
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|