QuantumPackage/src/tc_bi_ortho/tc_h_eigvectors.irp.f

  use bitmasks

 BEGIN_PROVIDER [ integer, index_HF_psi_det]                                                                                                            
 implicit none
 integer :: i,degree
 do i = 1, N_det
   call get_excitation_degree(HF_bitmask,psi_det(1,1,i),degree,N_int)
   if(degree == 0)then
    index_HF_psi_det = i
    exit
   endif
 enddo
 END_PROVIDER

subroutine diagonalize_CI_tc
  implicit none
  BEGIN_DOC
!  Replace the coefficients of the |CI| states by the coefficients of the
!  eigenstates of the |CI| matrix.
  END_DOC
  integer                        :: i,j
  do j=1,N_states
    do i=1,N_det
      psi_l_coef_bi_ortho(i,j) = leigvec_tc_bi_orth(i,j)
      psi_r_coef_bi_ortho(i,j) = reigvec_tc_bi_orth(i,j)
    enddo
  enddo
!  psi_energy(1:N_states) = CI_electronic_energy(1:N_states)
!  psi_s2(1:N_states) = CI_s2(1:N_states)

  SOFT_TOUCH psi_l_coef_bi_ortho psi_r_coef_bi_ortho
end



 BEGIN_PROVIDER [double precision, eigval_right_tc_bi_orth, (N_states)]
&BEGIN_PROVIDER [double precision, eigval_left_tc_bi_orth, (N_states)]
&BEGIN_PROVIDER [double precision, reigvec_tc_bi_orth, (N_det,N_states)]
&BEGIN_PROVIDER [double precision, leigvec_tc_bi_orth, (N_det,N_states)]
&BEGIN_PROVIDER [double precision, norm_ground_left_right_bi_orth ]

  BEGIN_DOC
  ! eigenvalues, right and left eigenvectors of the transcorrelated Hamiltonian on the BI-ORTHO basis 
  END_DOC

  implicit none
  integer                       :: i, idx_dress, j, istate
  logical                       :: converged, dagger
  integer                       :: n_real_tc_bi_orth_eigval_right,igood_r,igood_l
  integer,          allocatable :: iorder(:)
  double precision, allocatable :: reigvec_tc_bi_orth_tmp(:,:), leigvec_tc_bi_orth_tmp(:,:), eigval_right_tmp(:)
  double precision, allocatable :: coef_hf_r(:),coef_hf_l(:), Stmp(:,:)

  PROVIDE N_det N_int

  if(n_det .le. N_det_max_full) then

    allocate(reigvec_tc_bi_orth_tmp(N_det,N_det), leigvec_tc_bi_orth_tmp(N_det,N_det), eigval_right_tmp(N_det))

    call non_hrmt_real_diag( N_det, htilde_matrix_elmt_bi_ortho &
                           , leigvec_tc_bi_orth_tmp, reigvec_tc_bi_orth_tmp, n_real_tc_bi_orth_eigval_right, eigval_right_tmp)

    allocate(coef_hf_r(N_det), coef_hf_l(N_det), iorder(N_det))
    do i = 1, N_det
      iorder(i) = i
      coef_hf_r(i) = -dabs(reigvec_tc_bi_orth_tmp(index_HF_psi_det,i))
    enddo
    call dsort(coef_hf_r, iorder, N_det)
    igood_r = iorder(1)
    print*, 'igood_r, coef_hf_r = ', igood_r, coef_hf_r(1)
    do i = 1, N_det
     iorder(i) = i
     coef_hf_l(i) = -dabs(leigvec_tc_bi_orth_tmp(index_HF_psi_det,i))
    enddo
    call dsort(coef_hf_l, iorder, N_det)
    igood_l = iorder(1)
    print*, 'igood_l, coef_hf_l = ', igood_l, coef_hf_l(1)

    if(igood_r .ne. igood_l .and. igood_r .ne. 1)then
     print *,''
     print *,'Warning, the left and right eigenvectors are "not the same" '
     print *,'Warning, the ground state is not dominated by HF...'
     print *,'State with largest RIGHT coefficient of HF ',igood_r
     print *,'coef of HF in RIGHT eigenvector = ',reigvec_tc_bi_orth_tmp(index_HF_psi_det,igood_r)
     print *,'State with largest LEFT  coefficient of HF ',igood_l
     print *,'coef of HF in LEFT  eigenvector = ',leigvec_tc_bi_orth_tmp(index_HF_psi_det,igood_l)
    endif

    if(state_following_tc) then

     print *,'Following the states with the largest coef on HF'
     print *,'igood_r,igood_l',igood_r,igood_l
     i= igood_r
     eigval_right_tc_bi_orth(1) = eigval_right_tmp(i)
     do j = 1, N_det
       reigvec_tc_bi_orth(j,1) = reigvec_tc_bi_orth_tmp(j,i)
     enddo
     i= igood_l
     eigval_left_tc_bi_orth(1)  = eigval_right_tmp(i)
     do j = 1, N_det
       leigvec_tc_bi_orth(j,1) = leigvec_tc_bi_orth_tmp(j,i)
     enddo

    else 

      do i = 1, N_states
        eigval_right_tc_bi_orth(i) = eigval_right_tmp(i)
        eigval_left_tc_bi_orth(i)  = eigval_right_tmp(i)
        do j = 1, N_det
          reigvec_tc_bi_orth(j,i) = reigvec_tc_bi_orth_tmp(j,i)
          leigvec_tc_bi_orth(j,i) = leigvec_tc_bi_orth_tmp(j,i)
        enddo
      enddo

      ! check bi-orthogonality
      allocate(Stmp(N_states,N_states))
      call dgemm( 'T', 'N', N_states, N_states, N_det, 1.d0                                                              &
            , leigvec_tc_bi_orth(1,1), size(leigvec_tc_bi_orth, 1), reigvec_tc_bi_orth(1,1), size(reigvec_tc_bi_orth, 1) &
            , 0.d0, Stmp, size(Stmp, 1) )
      print *, ' overlap matrix between states:'
      do i = 1, N_states
        write(*,'(1000(F16.10,X))') Stmp(i,:)
      enddo
      deallocate(Stmp)

    endif

  else 

    double precision, allocatable :: H_jj(:),vec_tmp(:,:)
    external                         htc_bi_ortho_calc_tdav
    external                         htcdag_bi_ortho_calc_tdav
    external                         H_tc_u_0_opt
    external                         H_tc_dagger_u_0_opt
    allocate(H_jj(N_det),vec_tmp(N_det,n_states_diag))
    do i = 1, N_det
      call htilde_mu_mat_bi_ortho_tot(psi_det(1,1,i), psi_det(1,1,i), N_int, H_jj(i))
    enddo
 !!!! Preparing the left-eigenvector
    print*,'Computing the left-eigenvector '
    vec_tmp = 0.d0
    do istate = 1, N_states
     vec_tmp(1:N_det,istate) = psi_l_coef_bi_ortho(1:N_det,istate)
    enddo
    do istate = N_states+1, n_states_diag
     vec_tmp(istate,istate) = 1.d0
    enddo
!    call davidson_general_ext_rout_nonsym_b1space(vec_tmp, H_jj, eigval_left_tc_bi_orth, N_det, n_states, n_states_diag, converged, htcdag_bi_ortho_calc_tdav)
    call davidson_general_ext_rout_nonsym_b1space(vec_tmp, H_jj, eigval_left_tc_bi_orth, N_det, n_states, n_states_diag, converged, H_tc_dagger_u_0_opt)
    do istate = 1, N_states
     leigvec_tc_bi_orth(1:N_det,istate) = vec_tmp(1:N_det,istate)
    enddo

    print*,'Computing the right-eigenvector '
 !!!! Preparing the right-eigenvector
    vec_tmp = 0.d0
    do istate = 1, N_states
     vec_tmp(1:N_det,istate) = psi_r_coef_bi_ortho(1:N_det,istate)
    enddo
    do istate = N_states+1, n_states_diag
     vec_tmp(istate,istate) = 1.d0
    enddo
!    call davidson_general_ext_rout_nonsym_b1space(vec_tmp, H_jj, eigval_right_tc_bi_orth, N_det, n_states, n_states_diag, converged, htc_bi_ortho_calc_tdav)
    call davidson_general_ext_rout_nonsym_b1space(vec_tmp, H_jj, eigval_right_tc_bi_orth, N_det, n_states, n_states_diag, converged, H_tc_u_0_opt)
    do istate = 1, N_states
     reigvec_tc_bi_orth(1:N_det,istate) = vec_tmp(1:N_det,istate)
    enddo

    deallocate(H_jj)
   endif
  call bi_normalize(leigvec_tc_bi_orth,reigvec_tc_bi_orth,size(reigvec_tc_bi_orth,1),N_det,N_states)
   print*,'leigvec_tc_bi_orth(1,1),reigvec_tc_bi_orth(1,1) = ',leigvec_tc_bi_orth(1,1),reigvec_tc_bi_orth(1,1)
   norm_ground_left_right_bi_orth = 0.d0
   do j = 1, N_det
    norm_ground_left_right_bi_orth += leigvec_tc_bi_orth(j,1) * reigvec_tc_bi_orth(j,1)
   enddo
   print*,'norm l/r = ',norm_ground_left_right_bi_orth

END_PROVIDER 



subroutine bi_normalize(u_l,u_r,n,ld,nstates)
  !!!! Normalization of the scalar product of the left/right eigenvectors
  double precision, intent(inout) :: u_l(ld,nstates), u_r(ld,nstates)
  integer, intent(in) :: n,ld,nstates
  integer :: i
  double precision  :: accu, tmp 
  do i = 1, nstates
   !!!! Normalization of right eigenvectors |Phi>
   accu = 0.d0
   do j = 1, n
    accu += u_r(j,i) * u_r(j,i)
   enddo
   accu = 1.d0/dsqrt(accu)
   print*,'accu_r = ',accu
   do j = 1, n
    u_r(j,i) *= accu 
   enddo
   tmp = u_r(1,i) / dabs(u_r(1,i))
   do j = 1, n
    u_r(j,i) *= tmp
   enddo
   !!!! Adaptation of the norm of the left eigenvector such that <chi|Phi> = 1
   accu = 0.d0
   do j = 1, n
    accu += u_l(j,i) * u_r(j,i)
!    print*,j, u_l(j,i) , u_r(j,i)
   enddo
   if(accu.gt.0.d0)then
    accu = 1.d0/dsqrt(accu)
   else
    accu = 1.d0/dsqrt(-accu)
   endif
   tmp = (u_l(1,i) * u_r(1,i) )/dabs(u_l(1,i) * u_r(1,i))
   do j = 1, n
    u_l(j,i) *= accu * tmp
    u_r(j,i) *= accu 
   enddo
  enddo
end