Added the diagonalize_s2 option
This commit is contained in:
Emmanuel Giner
parent
2127503405
commit
6bbc24c1ec
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@ -24,7 +24,7 @@ python:
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script:
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- ./configure --production ./config/gfortran.cfg
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- source ./quantum_package.rc ; qp_module.py install Full_CI Hartree_Fock CAS_SD MRCC_CASSD
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- source ./quantum_package.rc ; qp_module.py install Full_CI Hartree_Fock CAS_SD MRCC_CASSD All_singles
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- source ./quantum_package.rc ; ninja
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- source ./quantum_package.rc ; cd ocaml ; make ; cd -
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- source ./quantum_package.rc ; cd tests ; bats bats/qp.bats
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@ -18,7 +18,7 @@ IRPF90_FLAGS : --ninja --align=32
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# 0 : Deactivate
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#
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[OPTION]
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MODE : OPT ; [ OPT | PROFILE | DEBUG ] : Chooses the section below
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MODE : DEBUG ; [ OPT | PROFILE | DEBUG ] : Chooses the section below
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CACHE : 1 ; Enable cache_compile.py
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OPENMP : 1 ; Append OpenMP flags
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@ -62,11 +62,27 @@ program full_ci
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endif
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print *, 'N_det = ', N_det
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print *, 'N_states = ', N_states
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do k = 1, N_states
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print*,'State ',k
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print *, 'PT2 = ', pt2
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print *, 'E = ', CI_energy
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print *, 'E(before)+PT2 = ', E_CI_before+pt2
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enddo
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print *, '-----'
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E_CI_before = CI_energy
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if(N_states.gt.1)then
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print*,'Variational Energy difference'
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do i = 2, N_states
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print*,'Delta E = ',CI_energy(i) - CI_energy(1)
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enddo
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endif
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if(N_states.gt.1)then
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print*,'Variational + perturbative Energy difference'
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do i = 2, N_states
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print*,'Delta E = ',E_CI_before(i)+ pt2(i) - (E_CI_before(1) + pt2(1))
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enddo
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endif
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E_CI_before = CI_energy
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call ezfio_set_full_ci_energy(CI_energy)
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if (abort_all) then
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exit
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@ -40,6 +40,12 @@ doc: Force the wave function to be an eigenfunction of S^2
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interface: ezfio,provider,ocaml
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default: False
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[diagonalize_s2]
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type: logical
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doc: Diagonalize the S^2 operator within the n_states_diag states required. Notice : the vectors are sorted by increasing S^2 values.
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interface: ezfio,provider,ocaml
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default: True
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[threshold_davidson]
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type: Threshold
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doc: Thresholds of Davidson's algorithm
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@ -36,17 +36,36 @@ END_PROVIDER
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BEGIN_PROVIDER [ double precision, CI_electronic_energy, (N_states_diag) ]
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&BEGIN_PROVIDER [ double precision, CI_eigenvectors, (N_det,N_states_diag) ]
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&BEGIN_PROVIDER [ double precision, CI_eigenvectors_s2, (N_states_diag) ]
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implicit none
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BEGIN_DOC
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! Eigenvectors/values of the CI matrix
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END_DOC
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integer :: i,j
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implicit none
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double precision :: ovrlp,u_dot_v
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integer :: i_good_state
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integer, allocatable :: index_good_state_array(:)
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logical, allocatable :: good_state_array(:)
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double precision, allocatable :: s2_values_tmp(:)
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integer :: i_other_state
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double precision, allocatable :: eigenvectors(:,:), eigenvalues(:)
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integer :: i_state
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double precision :: s2,e_0
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integer :: i,j,k
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double precision, allocatable :: s2_eigvalues(:)
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double precision, allocatable :: e_array(:)
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integer, allocatable :: iorder(:)
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do j=1,N_states_diag
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! Guess values for the "N_states_diag" states of the CI_eigenvectors
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do j=1,min(N_states_diag,N_det)
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do i=1,N_det
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CI_eigenvectors(i,j) = psi_coef(i,j)
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enddo
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enddo
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do j=N_det+1,N_states_diag
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do i=1,N_det
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CI_eigenvectors(i,j) = 0.d0
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enddo
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enddo
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if (diag_algorithm == "Davidson") then
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@ -59,36 +78,77 @@ END_PROVIDER
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else if (diag_algorithm == "Lapack") then
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double precision, allocatable :: eigenvectors(:,:), eigenvalues(:)
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allocate (eigenvectors(size(H_matrix_all_dets,1),N_det))
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allocate (eigenvalues(N_det))
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call lapack_diag(eigenvalues,eigenvectors, &
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H_matrix_all_dets,size(H_matrix_all_dets,1),N_det)
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CI_electronic_energy(:) = 0.d0
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do i=1,N_det
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CI_eigenvectors(i,1) = eigenvectors(i,1)
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enddo
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integer :: i_state
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double precision :: s2
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if (s2_eig) then
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i_state = 0
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allocate (s2_eigvalues(N_det))
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allocate(index_good_state_array(N_det),good_state_array(N_det))
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good_state_array = .False.
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do j=1,N_det
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call get_s2_u0(psi_det,eigenvectors(1,j),N_det,size(eigenvectors,1),s2)
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print*,'s2 = ',s2
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s2_eigvalues(j) = s2
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! Select at least n_states states with S^2 values closed to "expected_s2"
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if(dabs(s2-expected_s2).le.0.3d0)then
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i_state += 1
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do i=1,N_det
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CI_eigenvectors(i,i_state) = eigenvectors(i,j)
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enddo
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CI_electronic_energy(i_state) = eigenvalues(j)
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CI_eigenvectors_s2(i_state) = s2
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i_state +=1
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index_good_state_array(i_state) = j
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good_state_array(j) = .True.
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endif
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if (i_state.ge.N_states_diag) then
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exit
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if(i_state.eq.N_states) then
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exit
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endif
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enddo
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if(i_state .ne.0)then
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! Fill the first "i_state" states that have a correct S^2 value
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do j = 1, i_state
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do i=1,N_det
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CI_eigenvectors(i,j) = eigenvectors(i,index_good_state_array(j))
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enddo
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CI_electronic_energy(j) = eigenvalues(index_good_state_array(j))
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CI_eigenvectors_s2(j) = s2_eigvalues(index_good_state_array(j))
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enddo
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i_other_state = 0
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do j = 1, N_det
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if(good_state_array(j))cycle
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i_other_state +=1
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if(i_state+i_other_state.gt.n_states_diag)then
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exit
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endif
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call get_s2_u0(psi_det,eigenvectors(1,j),N_det,size(eigenvectors,1),s2)
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do i=1,N_det
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CI_eigenvectors(i,i_state+i_other_state) = eigenvectors(i,j)
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enddo
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CI_electronic_energy(i_state+i_other_state) = eigenvalues(j)
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CI_eigenvectors_s2(i_state+i_other_state) = s2
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enddo
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deallocate(index_good_state_array,good_state_array)
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else
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print*,''
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print*,'!!!!!!!! WARNING !!!!!!!!!'
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print*,' Within the ',N_det,'determinants selected'
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print*,' and the ',N_states_diag,'states requested'
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print*,' We did not find any state with S^2 values close to ',expected_s2
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print*,' We will then set the first N_states eigenvectors of the H matrix'
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print*,' as the CI_eigenvectors'
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print*,' You should consider more states and maybe ask for diagonalize_s2 to be .True. or just enlarge the CI space'
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print*,''
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do j=1,min(N_states_diag,N_det)
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do i=1,N_det
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CI_eigenvectors(i,j) = eigenvectors(i,j)
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enddo
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CI_electronic_energy(j) = eigenvalues(j)
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CI_eigenvectors_s2(j) = s2_eigvalues(j)
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enddo
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endif
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deallocate(s2_eigvalues)
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else
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do j=1,N_states_diag
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! Select the "N_states_diag" states of lowest energy
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do j=1,min(N_det,N_states_diag)
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call get_s2_u0(psi_det,eigenvectors(1,j),N_det,N_det,s2)
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do i=1,N_det
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CI_eigenvectors(i,j) = eigenvectors(i,j)
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@ -99,7 +159,100 @@ END_PROVIDER
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endif
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deallocate(eigenvectors,eigenvalues)
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endif
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if(diagonalize_s2.and.n_states_diag > 1.and. n_det >= n_states_diag)then
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! Diagonalizing S^2 within the "n_states_diag" states found
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allocate(s2_eigvalues(N_states_diag))
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call diagonalize_s2_betweenstates(psi_det,CI_eigenvectors,n_det,size(psi_det,3),size(CI_eigenvectors,1),min(n_states_diag,n_det),s2_eigvalues)
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do j = 1, N_states_diag
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do i = 1, N_det
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psi_coef(i,j) = CI_eigenvectors(i,j)
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enddo
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enddo
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if(s2_eig)then
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! Browsing the "n_states_diag" states and getting the lowest in energy "n_states" ones that have the S^2 value
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! closer to the "expected_s2" set as input
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allocate(index_good_state_array(N_det),good_state_array(N_det))
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good_state_array = .False.
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i_state = 0
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do j = 1, N_states_diag
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if(dabs(s2_eigvalues(j)-expected_s2).le.0.3d0)then
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good_state_array(j) = .True.
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i_state +=1
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index_good_state_array(i_state) = j
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endif
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enddo
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! Sorting the i_state good states by energy
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allocate(e_array(i_state),iorder(i_state))
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do j = 1, i_state
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do i = 1, N_det
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CI_eigenvectors(i,j) = psi_coef(i,index_good_state_array(j))
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enddo
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CI_eigenvectors_s2(j) = s2_eigvalues(index_good_state_array(j))
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call u0_H_u_0(e_0,CI_eigenvectors(1,j),n_det,psi_det,N_int)
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CI_electronic_energy(j) = e_0
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e_array(j) = e_0
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iorder(j) = j
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enddo
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call dsort(e_array,iorder,i_state)
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do j = 1, i_state
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CI_electronic_energy(j) = e_array(j)
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CI_eigenvectors_s2(j) = s2_eigvalues(index_good_state_array(iorder(j)))
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do i = 1, N_det
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CI_eigenvectors(i,j) = psi_coef(i,index_good_state_array(iorder(j)))
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enddo
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! call u0_H_u_0(e_0,CI_eigenvectors(1,j),n_det,psi_det,N_int)
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! print*,'e = ',CI_electronic_energy(j)
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! print*,'<e> = ',e_0
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! call get_s2_u0(psi_det,CI_eigenvectors(1,j),N_det,size(CI_eigenvectors,1),s2)
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! print*,'s^2 = ',CI_eigenvectors_s2(j)
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! print*,'<s^2>= ',s2
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enddo
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deallocate(e_array,iorder)
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! Then setting the other states without any specific energy order
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i_other_state = 0
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do j = 1, N_states_diag
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if(good_state_array(j))cycle
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i_other_state +=1
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do i = 1, N_det
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CI_eigenvectors(i,i_state + i_other_state) = psi_coef(i,j)
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enddo
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CI_eigenvectors_s2(i_state + i_other_state) = s2_eigvalues(j)
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call u0_H_u_0(e_0,CI_eigenvectors(1,i_state + i_other_state),n_det,psi_det,N_int)
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CI_electronic_energy(i_state + i_other_state) = e_0
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enddo
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deallocate(index_good_state_array,good_state_array)
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else
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! Sorting the N_states_diag by energy, whatever the S^2 value is
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allocate(e_array(n_states_diag),iorder(n_states_diag))
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do j = 1, N_states_diag
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call u0_H_u_0(e_0,CI_eigenvectors(1,j),n_det,psi_det,N_int)
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e_array(j) = e_0
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iorder(j) = j
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enddo
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call dsort(e_array,iorder,n_states_diag)
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do j = 1, N_states_diag
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CI_electronic_energy(j) = e_array(j)
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do i = 1, N_det
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CI_eigenvectors(i,j) = psi_coef(i,iorder(j))
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enddo
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CI_eigenvectors_s2(j) = s2_eigvalues(iorder(j))
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enddo
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deallocate(e_array,iorder)
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endif
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deallocate(s2_eigvalues)
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endif
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END_PROVIDER
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subroutine diagonalize_CI
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@ -214,4 +214,175 @@ subroutine get_s2_u0(psi_keys_tmp,psi_coefs_tmp,n,nmax,s2)
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deallocate (shortcut, sort_idx, sorted, version)
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end
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subroutine get_uJ_s2_uI(psi_keys_tmp,psi_coefs_tmp,n,nmax_coefs,nmax_keys,s2,nstates)
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implicit none
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use bitmasks
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integer(bit_kind), intent(in) :: psi_keys_tmp(N_int,2,nmax_keys)
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integer, intent(in) :: n,nmax_coefs,nmax_keys,nstates
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double precision, intent(in) :: psi_coefs_tmp(nmax_coefs,nstates)
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double precision, intent(out) :: s2(nstates,nstates)
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double precision :: s2_tmp,accu
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integer :: i,j,l,jj,ll,kk
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integer, allocatable :: idx(:)
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double precision, allocatable :: tmp(:,:)
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BEGIN_DOC
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! returns the matrix elements of S^2 "s2(i,j)" between the "nstates" states
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! psi_coefs_tmp(:,i) and psi_coefs_tmp(:,j)
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END_DOC
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s2 = 0.d0
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do ll = 1, nstates
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do jj = 1, nstates
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accu = 0.d0
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!$OMP PARALLEL DEFAULT(NONE) &
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!$OMP PRIVATE (i,j,kk,idx,tmp,s2_tmp) &
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!$OMP SHARED (ll,jj,psi_keys_tmp,psi_coefs_tmp,N_int,n,nstates) &
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!$OMP REDUCTION(+:accu)
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allocate(idx(0:n))
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!$OMP DO SCHEDULE(dynamic)
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do i = 1, n
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call get_s2(psi_keys_tmp(1,1,i),psi_keys_tmp(1,1,i),s2_tmp,N_int)
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accu += psi_coefs_tmp(i,ll) * s2_tmp * psi_coefs_tmp(i,jj)
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call filter_connected(psi_keys_tmp,psi_keys_tmp(1,1,i),N_int,i-1,idx)
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do kk=1,idx(0)
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j = idx(kk)
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call get_s2(psi_keys_tmp(1,1,i),psi_keys_tmp(1,1,j),s2_tmp,N_int)
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accu += psi_coefs_tmp(i,ll) * s2_tmp * psi_coefs_tmp(j,jj) + psi_coefs_tmp(i,jj) * s2_tmp * psi_coefs_tmp(j,ll)
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enddo
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enddo
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!$OMP END DO NOWAIT
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deallocate(idx)
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!$OMP BARRIER
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!$OMP END PARALLEL
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s2(ll,jj) += accu
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enddo
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enddo
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do i = 1, nstates
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do j =i+1,nstates
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accu = 0.5d0 * (s2(i,j) + s2(j,i))
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s2(i,j) = accu
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s2(j,i) = accu
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enddo
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enddo
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end
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subroutine diagonalize_s2_betweenstates(keys_tmp,psi_coefs_inout,n,nmax_keys,nmax_coefs,nstates,s2_eigvalues)
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BEGIN_DOC
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! You enter with nstates vectors in psi_coefs_inout that may be coupled by S^2
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! The subroutine diagonalize the S^2 operator in the basis of these states.
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! The vectors that you obtain in output are no more coupled by S^2,
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! which does not necessary mean that they are eigenfunction of S^2.
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! n,nmax,nstates = number of determinants, physical dimension of the arrays and number of states
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! keys_tmp = array of integer(bit_kind) that represents the determinants
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! psi_coefs(i,j) = coeff of the ith determinant in the jth state
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! VECTORS ARE SUPPOSED TO BE ORTHONORMAL IN INPUT
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END_DOC
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implicit none
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use bitmasks
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integer, intent(in) :: n,nmax_keys,nmax_coefs,nstates
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integer(bit_kind), intent(in) :: keys_tmp(N_int,2,nmax_keys)
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double precision, intent(inout) :: psi_coefs_inout(nmax_coefs,nstates)
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!integer, intent(in) :: ndets_real,ndets_keys,ndets_coefs,nstates
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!integer(bit_kind), intent(in) :: keys_tmp(N_int,2,ndets_keys)
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!double precision, intent(inout) :: psi_coefs_inout(ndets_coefs,nstates)
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double precision, intent(out) :: s2_eigvalues(nstates)
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double precision,allocatable :: s2(:,:),overlap(:,:)
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double precision, allocatable :: eigvalues(:),eigvectors(:,:)
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integer :: i,j,k
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double precision, allocatable :: psi_coefs_tmp(:,:)
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double precision :: accu,coef_contract
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double precision :: u_dot_u,u_dot_v
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print*,''
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print*,'*********************************************************************'
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print*,'Cleaning the various vectors by diagonalization of the S^2 matrix ...'
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print*,''
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print*,'nstates = ',nstates
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allocate(s2(nstates,nstates),overlap(nstates,nstates))
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do i = 1, nstates
|
||||
overlap(i,i) = u_dot_u(psi_coefs_inout(1,i),n)
|
||||
do j = i+1, nstates
|
||||
overlap(i,j) = u_dot_v(psi_coefs_inout(1,j),psi_coefs_inout(1,i),n)
|
||||
overlap(j,i) = overlap(i,j)
|
||||
enddo
|
||||
enddo
|
||||
print*,'Overlap matrix in the basis of the states considered'
|
||||
do i = 1, nstates
|
||||
write(*,'(10(F16.10,X))')overlap(i,:)
|
||||
enddo
|
||||
call ortho_lowdin(overlap,size(overlap,1),nstates,psi_coefs_inout,size(psi_coefs_inout,1),n)
|
||||
print*,'passed ortho'
|
||||
|
||||
do i = 1, nstates
|
||||
overlap(i,i) = u_dot_u(psi_coefs_inout(1,i),n)
|
||||
do j = i+1, nstates
|
||||
overlap(i,j) = u_dot_v(psi_coefs_inout(1,j),psi_coefs_inout(1,i),n)
|
||||
overlap(j,i) = overlap(i,j)
|
||||
enddo
|
||||
enddo
|
||||
print*,'Overlap matrix in the basis of the Lowdin orthonormalized states '
|
||||
do i = 1, nstates
|
||||
write(*,'(10(F16.10,X))')overlap(i,:)
|
||||
enddo
|
||||
|
||||
call get_uJ_s2_uI(keys_tmp,psi_coefs_inout,n_det,size(psi_coefs_inout,1),size(keys_tmp,3),s2,nstates)
|
||||
print*,'S^2 matrix in the basis of the states considered'
|
||||
double precision :: accu_precision_diag,accu_precision_of_diag
|
||||
accu_precision_diag = 0.d0
|
||||
accu_precision_of_diag = 0.d0
|
||||
do i = 1, nstates
|
||||
do j = i+1, nstates
|
||||
if( ( dabs(s2(i,i) - s2(j,j)) .le.1.d-10 ) .and. (dabs(s2(i,j) + dabs(s2(i,j)))) .le.1.d-10) then
|
||||
s2(i,j) = 0.d0
|
||||
s2(j,i) = 0.d0
|
||||
endif
|
||||
enddo
|
||||
enddo
|
||||
do i = 1, nstates
|
||||
write(*,'(10(F10.6,X))')s2(i,:)
|
||||
enddo
|
||||
|
||||
print*,'Diagonalizing the S^2 matrix'
|
||||
|
||||
allocate(eigvalues(nstates),eigvectors(nstates,nstates))
|
||||
call lapack_diagd(eigvalues,eigvectors,s2,nstates,nstates)
|
||||
print*,'Eigenvalues of s^2'
|
||||
do i = 1, nstates
|
||||
print*,'s2 = ',eigvalues(i)
|
||||
s2_eigvalues(i) = eigvalues(i)
|
||||
enddo
|
||||
|
||||
print*,'Building the eigenvectors of the S^2 matrix'
|
||||
allocate(psi_coefs_tmp(nmax_coefs,nstates))
|
||||
psi_coefs_tmp = 0.d0
|
||||
do j = 1, nstates
|
||||
do k = 1, nstates
|
||||
coef_contract = eigvectors(k,j) ! <phi_k|Psi_j>
|
||||
do i = 1, n_det
|
||||
psi_coefs_tmp(i,j) += psi_coefs_inout(i,k) * coef_contract
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
do j = 1, nstates
|
||||
accu = 0.d0
|
||||
do i = 1, n_det
|
||||
accu += psi_coefs_tmp(i,j) * psi_coefs_tmp(i,j)
|
||||
enddo
|
||||
print*,'Norm of vector = ',accu
|
||||
accu = 1.d0/dsqrt(accu)
|
||||
do i = 1, n_det
|
||||
psi_coefs_inout(i,j) = psi_coefs_tmp(i,j) * accu
|
||||
enddo
|
||||
enddo
|
||||
!call get_uJ_s2_uI(keys_tmp,psi_coefs_inout,n_det,size(psi_coefs_inout,1),size(keys_tmp,3),s2,nstates)
|
||||
!print*,'S^2 matrix in the basis of the NEW states considered'
|
||||
!do i = 1, nstates
|
||||
! write(*,'(10(F16.10,X))')s2(i,:)
|
||||
!enddo
|
||||
|
||||
deallocate(s2,eigvalues,eigvectors,psi_coefs_tmp,overlap)
|
||||
|
||||
end
|
||||
|
||||
|
|
|
|||
|
|
@ -1507,6 +1507,33 @@ subroutine get_occ_from_key(key,occ,Nint)
|
|||
|
||||
end
|
||||
|
||||
subroutine u0_H_u_0(e_0,u_0,n,keys_tmp,Nint)
|
||||
use bitmasks
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Computes e_0 = <u_0|H|u_0>/<u_0|u_0>
|
||||
!
|
||||
! n : number of determinants
|
||||
!
|
||||
END_DOC
|
||||
integer, intent(in) :: n,Nint
|
||||
double precision, intent(out) :: e_0
|
||||
double precision, intent(in) :: u_0(n)
|
||||
integer(bit_kind),intent(in) :: keys_tmp(Nint,2,n)
|
||||
|
||||
double precision :: H_jj(n)
|
||||
double precision :: v_0(n)
|
||||
double precision :: u_dot_u,u_dot_v,diag_H_mat_elem
|
||||
integer :: i,j
|
||||
do i = 1, n
|
||||
H_jj(i) = diag_H_mat_elem(keys_tmp(1,1,i),Nint)
|
||||
enddo
|
||||
|
||||
call H_u_0(v_0,u_0,H_jj,n,keys_tmp,Nint)
|
||||
e_0 = u_dot_v(v_0,u_0,n)/u_dot_u(u_0,n)
|
||||
end
|
||||
|
||||
|
||||
subroutine H_u_0(v_0,u_0,H_jj,n,keys_tmp,Nint)
|
||||
use bitmasks
|
||||
implicit none
|
||||
|
|
|
|||
Loading…
Reference in New Issue