wan_ham.F90 Source File


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sourcefile~~wan_ham.f90~~EfferentGraph sourcefile~wan_ham.f90 wan_ham.F90 sourcefile~utility.f90 utility.F90 sourcefile~wan_ham.f90->sourcefile~utility.f90 sourcefile~parameters.f90 parameters.F90 sourcefile~wan_ham.f90->sourcefile~parameters.f90 sourcefile~constants.f90 constants.F90 sourcefile~wan_ham.f90->sourcefile~constants.f90 sourcefile~io.f90 io.F90 sourcefile~wan_ham.f90->sourcefile~io.f90 sourcefile~get_oper.f90 get_oper.F90 sourcefile~wan_ham.f90->sourcefile~get_oper.f90 sourcefile~postw90_common.f90 postw90_common.F90 sourcefile~wan_ham.f90->sourcefile~postw90_common.f90 sourcefile~utility.f90->sourcefile~constants.f90 sourcefile~utility.f90->sourcefile~io.f90 sourcefile~parameters.f90->sourcefile~utility.f90 sourcefile~parameters.f90->sourcefile~constants.f90 sourcefile~parameters.f90->sourcefile~io.f90 sourcefile~comms.f90 comms.F90 sourcefile~parameters.f90->sourcefile~comms.f90 sourcefile~io.f90->sourcefile~constants.f90 sourcefile~get_oper.f90->sourcefile~utility.f90 sourcefile~get_oper.f90->sourcefile~parameters.f90 sourcefile~get_oper.f90->sourcefile~constants.f90 sourcefile~get_oper.f90->sourcefile~io.f90 sourcefile~get_oper.f90->sourcefile~postw90_common.f90 sourcefile~get_oper.f90->sourcefile~comms.f90 sourcefile~postw90_common.f90->sourcefile~utility.f90 sourcefile~postw90_common.f90->sourcefile~parameters.f90 sourcefile~postw90_common.f90->sourcefile~constants.f90 sourcefile~postw90_common.f90->sourcefile~io.f90 sourcefile~ws_distance.f90 ws_distance.F90 sourcefile~postw90_common.f90->sourcefile~ws_distance.f90 sourcefile~postw90_common.f90->sourcefile~comms.f90 sourcefile~ws_distance.f90->sourcefile~utility.f90 sourcefile~ws_distance.f90->sourcefile~parameters.f90 sourcefile~ws_distance.f90->sourcefile~constants.f90 sourcefile~ws_distance.f90->sourcefile~io.f90 sourcefile~comms.f90->sourcefile~constants.f90 sourcefile~comms.f90->sourcefile~io.f90

Files dependent on this one

sourcefile~~wan_ham.f90~~AfferentGraph sourcefile~wan_ham.f90 wan_ham.F90 sourcefile~geninterp.f90 geninterp.F90 sourcefile~geninterp.f90->sourcefile~wan_ham.f90 sourcefile~berry.f90 berry.F90 sourcefile~berry.f90->sourcefile~wan_ham.f90 sourcefile~gyrotropic.f90 gyrotropic.F90 sourcefile~gyrotropic.f90->sourcefile~wan_ham.f90 sourcefile~gyrotropic.f90->sourcefile~berry.f90 sourcefile~kslice.f90 kslice.F90 sourcefile~kslice.f90->sourcefile~wan_ham.f90 sourcefile~kslice.f90->sourcefile~berry.f90 sourcefile~boltzwann.f90 boltzwann.F90 sourcefile~boltzwann.f90->sourcefile~wan_ham.f90 sourcefile~dos.f90 dos.F90 sourcefile~boltzwann.f90->sourcefile~dos.f90 sourcefile~dos.f90->sourcefile~wan_ham.f90 sourcefile~kpath.f90 kpath.F90 sourcefile~kpath.f90->sourcefile~berry.f90 sourcefile~postw90.f90 postw90.F90 sourcefile~postw90.f90->sourcefile~geninterp.f90 sourcefile~postw90.f90->sourcefile~berry.f90 sourcefile~postw90.f90->sourcefile~gyrotropic.f90 sourcefile~postw90.f90->sourcefile~kslice.f90 sourcefile~postw90.f90->sourcefile~boltzwann.f90 sourcefile~postw90.f90->sourcefile~dos.f90 sourcefile~postw90.f90->sourcefile~kpath.f90

Contents

Source Code


Source Code

!-*- mode: F90 -*-!
!------------------------------------------------------------!
! This file is distributed as part of the Wannier90 code and !
! under the terms of the GNU General Public License. See the !
! file `LICENSE' in the root directory of the Wannier90      !
! distribution, or http://www.gnu.org/copyleft/gpl.txt       !
!                                                            !
! The webpage of the Wannier90 code is www.wannier.org       !
!                                                            !
! The Wannier90 code is hosted on GitHub:                    !
!                                                            !
! https://github.com/wannier-developers/wannier90            !
!------------------------------------------------------------!

module w90_wan_ham
  !! This module contain operations on the Hamiltonian in the WF basis

  use w90_constants, only: dp

  implicit none

  private

  public :: wham_get_D_h, wham_get_eig_deleig, wham_get_eig_deleig_TB_conv, wham_get_D_h_P_value
  public :: wham_get_occ_mat_list, wham_get_eig_UU_HH_JJlist
  public :: wham_get_eig_UU_HH_AA_sc, wham_get_eig_UU_HH_AA_sc_TB_conv

contains

  subroutine wham_get_D_h_a(delHH_a, UU, eig, ef, D_h_a)
    !===============================================!
    !                                               !
    !! Compute D^H_a=UU^dag.del_a UU (a=alpha,beta),
    !! using Eq.(24) of WYSV06
    !                                               !
    !===============================================!

    use w90_constants, only: dp, cmplx_0
    use w90_parameters, only: num_wann
    use w90_utility, only: utility_rotate
    use w90_postw90_common, only: pw90common_get_occ

    ! Arguments
    !
    complex(kind=dp), dimension(:, :), intent(in)  :: delHH_a
    complex(kind=dp), dimension(:, :), intent(in)  :: UU
    real(kind=dp), dimension(:), intent(in)  :: eig
    real(kind=dp), intent(in)  :: ef
    complex(kind=dp), dimension(:, :), intent(out) :: D_h_a

    complex(kind=dp), allocatable :: delHH_a_bar(:, :)
    real(kind=dp)                 :: occ(num_wann)
    integer                       :: n, m

    call pw90common_get_occ(eig, occ, ef)

    allocate (delHH_a_bar(num_wann, num_wann))
    delHH_a_bar = utility_rotate(delHH_a, UU, num_wann)
    do m = 1, num_wann
      do n = 1, num_wann
        if (occ(n) > 0.999_dp .and. occ(m) < 0.001_dp) then
          D_h_a(n, m) = delHH_a_bar(n, m)/(eig(m) - eig(n))
        else
          D_h_a(n, m) = cmplx_0
        end if
      end do
    end do
    D_h_a = D_h_a - conjg(transpose(D_h_a))

  end subroutine wham_get_D_h_a

  subroutine wham_get_D_h(delHH, UU, eig, D_h)
    !=========================================!
    !                                         !
    !! Compute D^H_a=UU^dag.del_a UU (a=x,y,z)
    !! using Eq.(24) of WYSV06
    !                                         !
    !=========================================!

    ! TO DO: Implement version where energy denominators only connect
    !        occupied and empty states. In this case probably do not need
    !        to worry about avoiding small energy denominators

    use w90_constants, only: dp, cmplx_0
    use w90_parameters, only: num_wann
    use w90_utility, only: utility_rotate

    ! Arguments
    !
    complex(kind=dp), dimension(:, :, :), intent(in)  :: delHH
    complex(kind=dp), dimension(:, :), intent(in)    :: UU
    real(kind=dp), dimension(:), intent(in)    :: eig
    complex(kind=dp), dimension(:, :, :), intent(out) :: D_h

    complex(kind=dp), allocatable :: delHH_bar_i(:, :)
    integer                       :: n, m, i

    allocate (delHH_bar_i(num_wann, num_wann))
    D_h = cmplx_0
    do i = 1, 3
      delHH_bar_i(:, :) = utility_rotate(delHH(:, :, i), UU, num_wann)
      do m = 1, num_wann
        do n = 1, num_wann
          if (n == m .or. abs(eig(m) - eig(n)) < 1.0e-7_dp) cycle
          D_h(n, m, i) = delHH_bar_i(n, m)/(eig(m) - eig(n))
        end do
      end do
    enddo

  end subroutine wham_get_D_h

  subroutine wham_get_D_h_P_value(delHH, UU, eig, D_h)
    !=========================================!
    !                                         !
    !! Compute D^H_a=UU^dag.del_a UU (a=x,y,z)
    !! using Eq.(24) of WYSV06
    !  and prescription for energy denominator
    !  from BK81
    !                                         !
    !=========================================!

    ! TO DO: Implement version where energy denominators only connect
    !        occupied and empty states. In this case probably do not need
    !        to worry about avoiding small energy denominators

    use w90_constants, only: dp, cmplx_0
    use w90_parameters, only: num_wann, sc_eta
    use w90_utility, only: utility_rotate

    ! Arguments
    !
    complex(kind=dp), dimension(:, :, :), intent(in)  :: delHH
    complex(kind=dp), dimension(:, :), intent(in)    :: UU
    real(kind=dp), dimension(:), intent(in)    :: eig
    complex(kind=dp), dimension(:, :, :), intent(out) :: D_h

    complex(kind=dp), allocatable :: delHH_bar_i(:, :)
    integer                       :: n, m, i
    real(kind=dp)                 :: deltaE

    allocate (delHH_bar_i(num_wann, num_wann))
    D_h = cmplx_0
    deltaE = 0.d0
    do i = 1, 3
      delHH_bar_i(:, :) = utility_rotate(delHH(:, :, i), UU, num_wann)
      do m = 1, num_wann
        do n = 1, num_wann
          if (n == m) cycle
          deltaE = eig(m) - eig(n)
          D_h(n, m, i) = delHH_bar_i(n, m)*(deltaE/(deltaE**(2) + sc_eta**(2)))
        end do
      end do
    enddo

  end subroutine wham_get_D_h_P_value

  subroutine wham_get_JJp_JJm_list(delHH, UU, eig, JJp_list, JJm_list, occ)
    !===============================================!
    !                                               !
    ! Compute JJ^+_a and JJ^-_a (a=Cartesian index) !
    ! for a list of Fermi energies                  !
    !                                               !
    ! This routine is a replacement for             !
    ! wham_get_JJp_list and wham_getJJm_list.       !
    ! It computes both lists at once in a more      !
    ! efficient manner.                             !
    !                                               !
    !  Tsirkin:   added the optional occ parameter  !
    !                                               !
    !===============================================!

    use w90_constants, only: dp, cmplx_0, cmplx_i
    use w90_parameters, only: num_wann, nfermi, fermi_energy_list
    use w90_utility, only: utility_rotate_new

    complex(kind=dp), dimension(:, :), intent(inout) :: delHH
    complex(kind=dp), dimension(:, :), intent(in)    :: UU
    real(kind=dp), dimension(:), intent(in)    :: eig
    complex(kind=dp), dimension(:, :, :), intent(out) :: JJp_list
    complex(kind=dp), dimension(:, :, :), intent(out) :: JJm_list
    real(kind=dp), intent(in), optional, dimension(:) :: occ

    integer                       :: n, m, ife, nfermi_loc
    real(kind=dp)                 :: fe

    if (present(occ)) then
      nfermi_loc = 1
    else
      nfermi_loc = nfermi
    endif

    call utility_rotate_new(delHH, UU, num_wann)
    do ife = 1, nfermi_loc
      fe = fermi_energy_list(ife)
      do m = 1, num_wann
        do n = 1, num_wann
          if (present(occ)) then
            if (occ(m) < 0.5_dp .and. occ(n) > 0.5_dp) then
              JJm_list(n, m, ife) = cmplx_i*delHH(n, m)/(eig(m) - eig(n))
              JJp_list(m, n, ife) = cmplx_i*delHH(m, n)/(eig(n) - eig(m))
            else
              JJm_list(n, m, ife) = cmplx_0
              JJp_list(m, n, ife) = cmplx_0
            end if
          else
            if (eig(n) > fe .and. eig(m) < fe) then
              JJp_list(n, m, ife) = cmplx_i*delHH(n, m)/(eig(m) - eig(n))
              JJm_list(m, n, ife) = cmplx_i*delHH(m, n)/(eig(n) - eig(m))
            else
              JJp_list(n, m, ife) = cmplx_0
              JJm_list(m, n, ife) = cmplx_0
            endif
          endif
        enddo
      enddo
      call utility_rotate_new(JJp_list(:, :, ife), UU, num_wann, reverse=.true.)
      call utility_rotate_new(JJm_list(:, :, ife), UU, num_wann, reverse=.true.)
    end do

  end subroutine wham_get_JJp_JJm_list

  subroutine wham_get_occ_mat_list(UU, f_list, g_list, eig, occ)
!  subroutine wham_get_occ_mat_list(eig,UU,f_list,g_list)
    !================================!
    !                                !
    !! Occupation matrix f, and g=1-f
    !! for a list of Fermi energies
    ! Tsirkin: !now optionally either eig or occ parameters may be supplied  !
    !    (Changed consistently the calls from the Berry module)        !
    !================================!

    use w90_constants, only: dp, cmplx_0, cmplx_1
    use w90_parameters, only: num_wann, nfermi, fermi_energy_list
    use w90_postw90_common, only: pw90common_get_occ
    use w90_io, only: io_error

    ! Arguments
    !
    complex(kind=dp), dimension(:, :), intent(in)  :: UU
    complex(kind=dp), dimension(:, :, :), intent(out) :: f_list
    complex(kind=dp), dimension(:, :, :), intent(out) :: g_list
    real(kind=dp), intent(in), optional, dimension(:) :: eig
    real(kind=dp), intent(in), optional, dimension(:) :: occ

    integer       :: n, m, i, if, nfermi_loc
    real(kind=dp), allocatable :: occ_list(:, :)

    if (present(occ)) then
      nfermi_loc = 1
    else
      nfermi_loc = nfermi
    endif
    allocate (occ_list(num_wann, nfermi_loc))

    if (present(occ) .and. present(eig)) then
      call io_error( &
        'occ_list and eig cannot be both arguments in get_occ_mat_list')
    elseif (.not. present(occ) .and. .not. present(eig)) then
      call io_error( &
        'either occ_list or eig must be passed as arguments to get_occ_mat_list')
    endif

    if (present(occ)) then
      occ_list(:, 1) = occ(:)
    else
      do if = 1, nfermi_loc
        call pw90common_get_occ(eig, occ_list(:, if), fermi_energy_list(if))
      enddo
    endif

    f_list = cmplx_0
    do if = 1, nfermi_loc
      do n = 1, num_wann
        do m = 1, num_wann
          do i = 1, num_wann
            f_list(n, m, if) = f_list(n, m, if) &
                               + UU(n, i)*occ_list(i, if)*conjg(UU(m, i))
          enddo
          g_list(n, m, if) = -f_list(n, m, if)
          if (m == n) g_list(n, n, if) = g_list(n, n, if) + cmplx_1
        enddo
      enddo
    enddo

  end subroutine wham_get_occ_mat_list

  subroutine wham_get_deleig_a(deleig_a, eig, delHH_a, UU)
    !==========================!
    !                          !
    !! Band derivatives dE/dk_a
    !                          !
    !==========================!

    use w90_constants, only: dp, cmplx_0, cmplx_i
    use w90_utility, only: utility_diagonalize, utility_rotate, &
      utility_rotate_diag
    use w90_parameters, only: num_wann, use_degen_pert, degen_thr

    ! Arguments
    !
    real(kind=dp), intent(out) :: deleig_a(num_wann)
    real(kind=dp), intent(in)  :: eig(num_wann)
    complex(kind=dp), dimension(:, :), intent(in)  :: delHH_a
    complex(kind=dp), dimension(:, :), intent(in)  :: UU

    ! Misc/Dummy
    !
    integer                       :: i, degen_min, degen_max, dim
    real(kind=dp)                 :: diff
    complex(kind=dp), allocatable :: delHH_bar_a(:, :), U_deg(:, :)

    allocate (delHH_bar_a(num_wann, num_wann))
    allocate (U_deg(num_wann, num_wann))

    if (use_degen_pert) then

      delHH_bar_a = utility_rotate(delHH_a, UU, num_wann)

      ! Assuming that the energy eigenvalues are stored in eig(:) in
      ! increasing order (diff >= 0)

      i = 0
      do
        i = i + 1
        if (i > num_wann) exit
        if (i + 1 <= num_wann) then
          diff = eig(i + 1) - eig(i)
        else
          !
          ! i-th is the highest band, and it is non-degenerate
          !
          diff = degen_thr + 1.0_dp
        end if
        if (diff < degen_thr) then
          !
          ! Bands i and i+1 are degenerate
          !
          degen_min = i
          degen_max = degen_min + 1
          !
          ! See if any higher bands are in the same degenerate group
          !
          do
            if (degen_max + 1 > num_wann) exit
            diff = eig(degen_max + 1) - eig(degen_max)
            if (diff < degen_thr) then
              degen_max = degen_max + 1
            else
              exit
            end if
          end do
          !
          ! Bands from degen_min to degen_max are degenerate. Diagonalize
          ! the submatrix in Eq.(31) YWVS07 over this degenerate subspace.
          ! The eigenvalues are the band gradients
          !
          !
          dim = degen_max - degen_min + 1
          call utility_diagonalize(delHH_bar_a(degen_min:degen_max, &
                                               degen_min:degen_max), dim, &
                                   deleig_a(degen_min:degen_max), U_deg(1:dim, 1:dim))
          !
          ! Scanned bands up to degen_max
          !
          i = degen_max
        else
          !
          ! Use non-degenerate form [Eq.(27) YWVS07] for current (i-th) band
          !
          deleig_a(i) = real(delHH_bar_a(i, i), dp)
        end if
      end do

    else

      ! Use non-degenerate form for all bands
      !
      deleig_a(:) = real(utility_rotate_diag(delHH_a(:, :), UU, num_wann), dp)

    end if

  end subroutine wham_get_deleig_a

  subroutine wham_get_eig_deleig(kpt, eig, del_eig, HH, delHH, UU)
    !! Given a k point, this function returns eigenvalues E and
    !! derivatives of the eigenvalues dE/dk_a, using wham_get_deleig_a
    !
    use w90_parameters, only: num_wann
    use w90_get_oper, only: HH_R, get_HH_R
    use w90_postw90_common, only: pw90common_fourier_R_to_k
    use w90_utility, only: utility_diagonalize

    real(kind=dp), dimension(3), intent(in)         :: kpt
    !! the three coordinates of the k point vector (in relative coordinates)
    real(kind=dp), intent(out)                      :: eig(num_wann)
    !! the calculated eigenvalues at kpt
    real(kind=dp), intent(out)                      :: del_eig(num_wann, 3)
    !! the calculated derivatives of the eigenvalues at kpt [first component: band; second component: 1,2,3
    !! for the derivatives along the three k directions]
    complex(kind=dp), dimension(:, :), intent(out)   :: HH
    !! the Hamiltonian matrix at kpt
    complex(kind=dp), dimension(:, :, :), intent(out) :: delHH
    !! the delHH matrix (derivative of H) at kpt
    complex(kind=dp), dimension(:, :), intent(out)   :: UU
    !! the rotation matrix that gives the eigenvectors of HH

    ! I call it to be sure that it has been called already once,
    ! and that HH_R contains the actual matrix.
    ! Further calls should return very fast.
    call get_HH_R

    call pw90common_fourier_R_to_k(kpt, HH_R, HH, 0)
    call utility_diagonalize(HH, num_wann, eig, UU)
    call pw90common_fourier_R_to_k(kpt, HH_R, delHH(:, :, 1), 1)
    call pw90common_fourier_R_to_k(kpt, HH_R, delHH(:, :, 2), 2)
    call pw90common_fourier_R_to_k(kpt, HH_R, delHH(:, :, 3), 3)
    call wham_get_deleig_a(del_eig(:, 1), eig, delHH(:, :, 1), UU)
    call wham_get_deleig_a(del_eig(:, 2), eig, delHH(:, :, 2), UU)
    call wham_get_deleig_a(del_eig(:, 3), eig, delHH(:, :, 3), UU)

  end subroutine wham_get_eig_deleig

  subroutine wham_get_eig_deleig_TB_conv(kpt, eig, del_eig, delHH, UU)
    ! modified version of wham_get_eig_deleig for the TB convention
    ! avoids recalculating delHH and UU, works with input values

    !! Given a k point, this function returns eigenvalues E and
    !! derivatives of the eigenvalues dE/dk_a, using wham_get_deleig_a
    !
    use w90_parameters, only: num_wann
    use w90_get_oper, only: HH_R, get_HH_R
    use w90_postw90_common, only: pw90common_fourier_R_to_k
    use w90_utility, only: utility_diagonalize

    real(kind=dp), dimension(3), intent(in)         :: kpt
    !! the three coordinates of the k point vector (in relative coordinates)
    real(kind=dp), intent(out)                      :: del_eig(num_wann, 3)
    real(kind=dp), intent(in)                      :: eig(num_wann)
    complex(kind=dp), dimension(:, :, :), intent(in) :: delHH
    !! the delHH matrix (derivative of H) at kpt
    complex(kind=dp), dimension(:, :), intent(in)   :: UU
    !! the rotation matrix that gives the eigenvectors of HH

    call wham_get_deleig_a(del_eig(:, 1), eig, delHH(:, :, 1), UU)
    call wham_get_deleig_a(del_eig(:, 2), eig, delHH(:, :, 2), UU)
    call wham_get_deleig_a(del_eig(:, 3), eig, delHH(:, :, 3), UU)

  end subroutine wham_get_eig_deleig_TB_conv

  subroutine wham_get_eig_UU_HH_JJlist(kpt, eig, UU, HH, JJp_list, JJm_list, occ)
    !========================================================!
    !                                                        !
    !! Wrapper routine used to reduce number of Fourier calls
    !    Added the optional occ parameter                    !
    !========================================================!

    use w90_parameters, only: num_wann
    use w90_get_oper, only: HH_R, get_HH_R
    use w90_postw90_common, only: pw90common_fourier_R_to_k_new
    use w90_utility, only: utility_diagonalize

    real(kind=dp), dimension(3), intent(in)           :: kpt
    real(kind=dp), intent(out)                        :: eig(num_wann)
    complex(kind=dp), dimension(:, :), intent(out)     :: UU
    complex(kind=dp), dimension(:, :), intent(out)     :: HH
    complex(kind=dp), dimension(:, :, :, :), intent(out) :: JJp_list
    complex(kind=dp), dimension(:, :, :, :), intent(out) :: JJm_list
    real(kind=dp), intent(in), optional, dimension(:) :: occ

    integer                       :: i
    complex(kind=dp), allocatable :: delHH(:, :, :)

    call get_HH_R

    allocate (delHH(num_wann, num_wann, 3))
    call pw90common_fourier_R_to_k_new(kpt, HH_R, OO=HH, &
                                       OO_dx=delHH(:, :, 1), &
                                       OO_dy=delHH(:, :, 2), &
                                       OO_dz=delHH(:, :, 3))
    call utility_diagonalize(HH, num_wann, eig, UU)
    do i = 1, 3
      if (present(occ)) then
        call wham_get_JJp_JJm_list(delHH(:, :, i), UU, eig, JJp_list(:, :, :, i), JJm_list(:, :, :, i), occ=occ)
      else
        call wham_get_JJp_JJm_list(delHH(:, :, i), UU, eig, JJp_list(:, :, :, i), JJm_list(:, :, :, i))
      endif
    enddo

  end subroutine wham_get_eig_UU_HH_JJlist

  subroutine wham_get_eig_UU_HH_AA_sc_TB_conv(kpt, eig, UU, HH, HH_da, HH_dadb)
    !========================================================!
    !                                                        !
    ! modified version of wham_get_eig_UU_HH_AA_sc, calls routines
    ! satisfying the TB phase convention
    !                                                        !
    !========================================================!

    use w90_parameters, only: num_wann
    use w90_get_oper, only: HH_R, get_HH_R, AA_R, get_AA_R
    use w90_postw90_common, only: pw90common_fourier_R_to_k_new_second_d, &
      pw90common_fourier_R_to_k_new_second_d_TB_conv
    use w90_utility, only: utility_diagonalize

    real(kind=dp), dimension(3), intent(in)           :: kpt
    real(kind=dp), intent(out)                        :: eig(num_wann)
    complex(kind=dp), dimension(:, :), intent(out)     :: UU
    complex(kind=dp), dimension(:, :), intent(out)     :: HH
    complex(kind=dp), dimension(:, :, :), intent(out)       :: HH_da
    complex(kind=dp), dimension(:, :, :, :), intent(out)     :: HH_dadb

    integer                       :: i

    call get_HH_R
    call get_AA_R

    call pw90common_fourier_R_to_k_new_second_d_TB_conv(kpt, HH_R, AA_R, OO=HH, &
                                                        OO_da=HH_da(:, :, :), &
                                                        OO_dadb=HH_dadb(:, :, :, :))
    call utility_diagonalize(HH, num_wann, eig, UU)

  end subroutine wham_get_eig_UU_HH_AA_sc_TB_conv

  subroutine wham_get_eig_UU_HH_AA_sc(kpt, eig, UU, HH, HH_da, HH_dadb)
    !========================================================!
    !                                                        !
    !! Wrapper routine used to reduce number of Fourier calls
    !                                                        !
    !========================================================!

    use w90_parameters, only: num_wann
    use w90_get_oper, only: HH_R, get_HH_R
    use w90_postw90_common, only: pw90common_fourier_R_to_k_new_second_d
    use w90_utility, only: utility_diagonalize

    real(kind=dp), dimension(3), intent(in)           :: kpt
    real(kind=dp), intent(out)                        :: eig(num_wann)
    complex(kind=dp), dimension(:, :), intent(out)     :: UU
    complex(kind=dp), dimension(:, :), intent(out)     :: HH
    complex(kind=dp), dimension(:, :, :), intent(out)       :: HH_da
    complex(kind=dp), dimension(:, :, :, :), intent(out)     :: HH_dadb

    integer                       :: i

    call get_HH_R

    call pw90common_fourier_R_to_k_new_second_d(kpt, HH_R, OO=HH, &
                                                OO_da=HH_da(:, :, :), &
                                                OO_dadb=HH_dadb(:, :, :, :))
    call utility_diagonalize(HH, num_wann, eig, UU)

  end subroutine wham_get_eig_UU_HH_AA_sc

end module w90_wan_ham