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199 lines
6.3 KiB
Fortran
199 lines
6.3 KiB
Fortran
subroutine H_tc_s2_u_0_with_pure_three(v_0, s_0, u_0, N_st, sze)
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BEGIN_DOC
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! Computes $v_0 = H^TC | u_0\rangle$ WITH PURE TRIPLE EXCITATION TERMS
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!
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! Assumes that the determinants are in psi_det
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!
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! istart, iend, ishift, istep are used in ZMQ parallelization.
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END_DOC
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use bitmasks
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implicit none
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integer, intent(in) :: N_st,sze
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double precision, intent(in) :: u_0(sze,N_st)
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double precision, intent(out) :: v_0(sze,N_st), s_0(sze,N_st)
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call H_tc_s2_u_0_opt(v_0, s_0, u_0, N_st, sze)
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integer :: i,j,degree,ist
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double precision :: hmono, htwoe, hthree, htot
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do i = 1, N_det
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do j = 1, N_det
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call get_excitation_degree(psi_det(1,1,i),psi_det(1,1,j),degree,N_int)
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if(degree .ne. 3)cycle
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call triple_htilde_mu_mat_fock_bi_ortho(N_int, psi_det(1,1,i), psi_det(1,1,j), hmono, htwoe, hthree, htot)
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do ist = 1, N_st
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v_0(i,ist) += htot * u_0(j,ist)
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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 H_tc_s2_u_0_with_pure_three_omp(v_0, s_0, u_0, N_st, sze)
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BEGIN_DOC
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! Computes $v_0 = H^TC | u_0\rangle$ WITH PURE TRIPLE EXCITATION TERMS
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!
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! Assumes that the determinants are in psi_det
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!
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! istart, iend, ishift, istep are used in ZMQ parallelization.
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END_DOC
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use bitmasks
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implicit none
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integer, intent(in) :: N_st,sze
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double precision, intent(in) :: u_0(sze,N_st)
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double precision, intent(out) :: v_0(sze,N_st), s_0(sze,N_st)
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call H_tc_s2_u_0_opt(v_0, s_0, u_0, N_st, sze)
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integer :: i,j,degree,ist
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double precision :: hmono, htwoe, hthree, htot
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!$OMP PARALLEL DO DEFAULT(NONE) SCHEDULE(dynamic,8) &
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!$OMP SHARED(N_st, N_det, N_int, psi_det, u_0, v_0) &
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!$OMP PRIVATE(ist, i, j, degree, hmono, htwoe, hthree,htot)
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do i = 1, N_det
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do j = 1, N_det
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call get_excitation_degree(psi_det(1,1,i),psi_det(1,1,j),degree,N_int)
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if(degree .ne. 3)cycle
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call triple_htilde_mu_mat_fock_bi_ortho(N_int, psi_det(1,1,i), psi_det(1,1,j), hmono, htwoe, hthree, htot)
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do ist = 1, N_st
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v_0(i,ist) += htot * u_0(j,ist)
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enddo
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enddo
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enddo
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!$OMP END PARALLEL DO
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end
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! ---
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subroutine H_tc_s2_dagger_u_0_with_pure_three(v_0, s_0, u_0, N_st, sze)
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BEGIN_DOC
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! Computes $v_0 = (H^TC)^dagger | u_0\rangle$ WITH PURE TRIPLE EXCITATION TERMS
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!
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! Assumes that the determinants are in psi_det
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!
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! istart, iend, ishift, istep are used in ZMQ parallelization.
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END_DOC
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use bitmasks
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implicit none
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integer, intent(in) :: N_st,sze
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double precision, intent(in) :: u_0(sze,N_st)
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double precision, intent(out) :: v_0(sze,N_st), s_0(sze,N_st)
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call H_tc_s2_dagger_u_0_opt(v_0, s_0, u_0, N_st, sze)
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integer :: i,j,degree,ist
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double precision :: hmono, htwoe, hthree, htot
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do i = 1, N_det
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do j = 1, N_det
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call get_excitation_degree(psi_det(1,1,i),psi_det(1,1,j),degree,N_int)
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if(degree .ne. 3)cycle
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call triple_htilde_mu_mat_fock_bi_ortho(N_int, psi_det(1,1,j), psi_det(1,1,i), hmono, htwoe, hthree, htot)
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do ist = 1, N_st
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v_0(i,ist) += htot * u_0(j,ist)
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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 H_tc_s2_dagger_u_0_with_pure_three_omp(v_0, s_0, u_0, N_st, sze)
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BEGIN_DOC
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! Computes $v_0 = (H^TC)^dagger | u_0\rangle$ WITH PURE TRIPLE EXCITATION TERMS
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!
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! Assumes that the determinants are in psi_det
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!
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! istart, iend, ishift, istep are used in ZMQ parallelization.
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END_DOC
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use bitmasks
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implicit none
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integer, intent(in) :: N_st,sze
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double precision, intent(in) :: u_0(sze,N_st)
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double precision, intent(out) :: v_0(sze,N_st), s_0(sze,N_st)
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call H_tc_s2_dagger_u_0_opt(v_0, s_0, u_0, N_st, sze)
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integer :: i,j,degree,ist
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double precision :: hmono, htwoe, hthree, htot
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!$OMP PARALLEL DO DEFAULT(NONE) SCHEDULE(dynamic,8) &
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!$OMP SHARED(N_st, N_det, N_int, psi_det, u_0, v_0) &
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!$OMP PRIVATE(ist, i, j, degree, hmono, htwoe, hthree,htot)
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do i = 1, N_det
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do j = 1, N_det
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call get_excitation_degree(psi_det(1,1,i),psi_det(1,1,j),degree,N_int)
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if(degree .ne. 3)cycle
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call triple_htilde_mu_mat_fock_bi_ortho(N_int, psi_det(1,1,j), psi_det(1,1,i), hmono, htwoe, hthree, htot)
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do ist = 1, N_st
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v_0(i,ist) += htot * u_0(j,ist)
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enddo
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enddo
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enddo
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!$OMP END PARALLEL DO
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end
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! ---
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subroutine triple_htilde_mu_mat_fock_bi_ortho(Nint, key_j, key_i, hmono, htwoe, hthree, htot)
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use bitmasks
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BEGIN_DOC
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! <key_j | H_tilde | key_i> for triple excitation
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!!
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!! WARNING !!
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!
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! Genuine triple excitations of the same spin are not yet implemented
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END_DOC
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implicit none
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integer(bit_kind), intent(in) :: key_j(N_int,2),key_i(N_int,2)
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integer, intent(in) :: Nint
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double precision, intent(out) :: hmono, htwoe, hthree, htot
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integer :: degree
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integer :: h1, p1, h2, p2, s1, s2, h3, p3, s3
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integer :: holes_array(100,2),particles_array(100,2),degree_array(2)
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double precision :: phase,sym_3_e_int_from_6_idx_tensor
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hmono = 0.d0
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htwoe = 0.d0
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hthree = 0.d0
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htot = 0.d0
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call get_excitation_general(key_j, key_i, Nint,degree_array,holes_array, particles_array,phase)
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degree = degree_array(1) + degree_array(2)
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if(degree .ne. 3)return
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if(degree_array(1)==3.or.degree_array(2)==3)then
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if(degree_array(1) == 3)then
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h1 = holes_array(1,1)
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h2 = holes_array(2,1)
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h3 = holes_array(3,1)
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p1 = particles_array(1,1)
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p2 = particles_array(2,1)
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p3 = particles_array(3,1)
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else
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h1 = holes_array(1,2)
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h2 = holes_array(2,2)
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h3 = holes_array(3,2)
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p1 = particles_array(1,2)
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p2 = particles_array(2,2)
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p3 = particles_array(3,2)
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endif
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hthree = sym_3_e_int_from_6_idx_tensor(p3, p2, p1, h3, h2, h1)
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else
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if(degree_array(1) == 2.and.degree_array(2) == 1)then ! double alpha + single beta
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h1 = holes_array(1,1)
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h2 = holes_array(2,1)
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h3 = holes_array(1,2)
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p1 = particles_array(1,1)
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p2 = particles_array(2,1)
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p3 = particles_array(1,2)
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else if(degree_array(2) == 2 .and. degree_array(1) == 1)then ! double beta + single alpha
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h1 = holes_array(1,2)
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h2 = holes_array(2,2)
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h3 = holes_array(1,1)
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p1 = particles_array(1,2)
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p2 = particles_array(2,2)
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p3 = particles_array(1,1)
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else
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print*,'PB !!'
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stop
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endif
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hthree = three_body_ints_bi_ort(p3,p2,p1,h3,h2,h1) - three_body_ints_bi_ort(p3,p2,p1,h3,h1,h2)
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endif
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hthree *= phase
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htot = hthree
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end
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