mirror of https://gitlab.com/QEF/q-e.git
875 lines
25 KiB
Fortran
875 lines
25 KiB
Fortran
!
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! Copyright (C) 2001-2005 Quantum-ESPRESSO group
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! This file is distributed under the terms of the
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! GNU General Public License. See the file `License'
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! in the root directory of the present distribution,
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! or http://www.gnu.org/copyleft/gpl.txt .
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!
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#define ZERO ( 0.D0, 0.D0 )
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#define ONE ( 1.D0, 0.D0 )
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!
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#include "f_defs.h"
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!
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!----------------------------------------------------------------------------
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SUBROUTINE cegterg( ndim, ndmx, nvec, nvecx, evc, ethr, &
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uspp, e, btype, notcnv, lrot, dav_iter )
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!----------------------------------------------------------------------------
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!
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! ... iterative solution of the eigenvalue problem:
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!
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! ... ( H - e S ) * evc = 0
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!
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! ... where H is an hermitean operator, e is a real scalar,
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! ... S is an uspp matrix, evc is a complex vector
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!
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USE io_global, ONLY : stdout
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USE kinds, ONLY : DP
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USE control_flags, ONLY : use_para_diago
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USE noncollin_module, ONLY : noncolin, npol
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USE bp, ONLY : lelfield
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!
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IMPLICIT NONE
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!
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! ... on INPUT
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!
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INTEGER, INTENT(IN) :: ndim, ndmx, nvec, nvecx
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! dimension of the matrix to be diagonalized
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! leading dimension of matrix evc, as declared in the calling pgm unit
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! integer number of searched low-lying roots
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! maximum dimension of the reduced basis set :
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! (the basis set is refreshed when its dimension would exceed nvecx)
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! k-point considered
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COMPLEX(DP), INTENT(INOUT) :: evc(ndmx,npol,nvec)
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! evc contains the refined estimates of the eigenvectors
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REAL(DP), INTENT(IN) :: ethr
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! energy threshold for convergence :
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! root improvement is stopped, when two consecutive estimates of the root
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! differ by less than ethr.
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LOGICAL, INTENT(IN) :: uspp
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! if .FALSE. : do not calculate S|psi>
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INTEGER, INTENT(IN) :: btype(nvec)
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! band type ( 1 = occupied, 0 = empty )
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LOGICAL, INTENT(IN) :: lrot
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! .TRUE. if the wfc have already been rotated
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!
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! ... on OUTPUT
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!
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REAL(DP), INTENT(OUT) :: e(nvec)
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! contains the estimated roots.
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INTEGER, INTENT(OUT) :: dav_iter, notcnv
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! integer number of iterations performed
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! number of unconverged roots
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!
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! ... LOCAL variables
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!
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INTEGER, PARAMETER :: maxter = 20
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! maximum number of iterations
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!
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INTEGER :: kter, nbase, np, kdim, kdmx, n, m, nb1, nbn
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! counter on iterations
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! dimension of the reduced basis
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! counter on the reduced basis vectors
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! adapted ndim and ndmx
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! do-loop counters
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COMPLEX(DP), ALLOCATABLE :: hc(:,:), sc(:,:), vc(:,:)
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! Hamiltonian on the reduced basis
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! S matrix on the reduced basis
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! the eigenvectors of the Hamiltonian
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COMPLEX(DP), ALLOCATABLE :: psi(:,:,:), hpsi(:,:,:), spsi(:,:,:)
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! work space, contains psi
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! the product of H and psi
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! the product of S and psi
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REAL(DP), ALLOCATABLE :: ew(:)
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! eigenvalues of the reduced hamiltonian
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LOGICAL, ALLOCATABLE :: conv(:)
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! true if the root is converged
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REAL(DP) :: empty_ethr
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! threshold for empty bands
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!
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! ... Called routines:
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!
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REAL(DP), EXTERNAL :: DDOT
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!
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EXTERNAL h_psi, s_psi, g_psi
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EXTERNAL h_psi_nc, s_psi_nc, g_psi_nc
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! h_psi(ndmx,ndim,nvec,psi,hpsi)
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! calculates H|psi>
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! s_psi(ndmx,ndim,nvec,spsi)
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! calculates S|psi> (if needed)
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! Vectors psi,hpsi,spsi are dimensioned (ndmx,npol,nvec)
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! g_psi(ndmx,ndim,notcnv,psi,e)
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! calculates (diag(h)-e)^-1 * psi, diagonal approx. to (h-e)^-1*psi
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! the first nvec columns contain the trial eigenvectors
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!
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!
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CALL start_clock( 'cegterg' )
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!
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IF ( nvec > nvecx / 2 ) CALL errore( 'cegter', 'nvecx is too small', 1 )
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!
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! ... threshold for empty bands
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!
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empty_ethr = MAX( ( ethr * 5.D0 ), 1.D-5 )
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!
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IF ( npol == 1 ) THEN
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!
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kdim = ndim
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kdmx = ndmx
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!
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ELSE
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!
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kdim = ndmx*npol
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kdmx = ndmx*npol
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!
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END IF
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!
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IF ( use_para_diago ) THEN
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!
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CALL cegterg_para()
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!
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ELSE
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!
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CALL cegterg_serial()
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!
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END IF
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!
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CALL stop_clock( 'cegterg' )
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!
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RETURN
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!
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CONTAINS
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!
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!------------------------------------------------------------------------
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SUBROUTINE cegterg_para()
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!------------------------------------------------------------------------
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!
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IMPLICIT NONE
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!
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! ... allocate the work arrays
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!
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ALLOCATE( psi( ndmx, npol, nvecx ) )
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ALLOCATE( hpsi( ndmx, npol, nvecx ) )
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ALLOCATE( spsi( ndmx, npol, nvecx ) )
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ALLOCATE( hc( nvecx, nvecx ) )
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ALLOCATE( vc( nvecx, nvecx ) )
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ALLOCATE( ew( nvecx ) )
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ALLOCATE( conv( nvec ) )
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!
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notcnv = nvec
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nbase = nvec
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conv = .FALSE.
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!
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spsi = ZERO
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hpsi = ZERO
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psi = ZERO
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psi(:,:,1:nvec) = evc(:,:,1:nvec)
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!
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! ... hpsi contains H times the basis vectors
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!
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IF ( noncolin ) THEN
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!
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CALL h_psi_nc( ndmx, ndim, nvec, psi, hpsi )
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!
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IF ( lelfield ) CALL h_epsi_her( ndmx, ndim, nvec, psi, hpsi )
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!
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IF ( uspp ) THEN
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!
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CALL s_psi_nc( ndmx, ndim, nvec, psi, spsi )
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!
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ELSE
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!
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spsi(:,:,:) = psi(:,:,:)
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!
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END IF
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!
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CALL cgramg1_nc( ndmx, nvecx, ndim, 1, nvec, psi, spsi, hpsi, npol )
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!
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ELSE
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!
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CALL h_psi( ndmx, ndim, nvec, psi, hpsi )
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!
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IF ( lelfield ) CALL h_epsi_her( ndmx, ndim, nvec, psi, hpsi )
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!
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IF ( uspp ) THEN
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!
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CALL s_psi( ndmx, ndim, nvec, psi, spsi )
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!
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ELSE
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!
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spsi(:,:,:) = psi(:,:,:)
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!
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END IF
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!
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CALL cgramg1( kdmx, nvecx, kdim, 1, nvec, psi, spsi, hpsi )
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!
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END IF
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!
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! ... hc contains the projection of the hamiltonian onto the reduced
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! ... space vc contains the eigenvectors of hc
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!
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hc(:,:) = ZERO
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vc(:,:) = ZERO
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!
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CALL ZGEMM( 'C', 'N', nbase, nbase, kdim, ONE, &
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psi, kdmx, hpsi, kdmx, ZERO, hc, nvecx )
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!
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CALL reduce( 2*nbase*nvecx, hc )
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!
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IF ( lrot ) THEN
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!
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DO n = 1, nbase
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!
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e(n) = REAL( hc(n,n) )
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!
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vc(n,n) = ONE
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!
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END DO
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!
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ELSE
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!
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! ... diagonalize the reduced hamiltonian
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!
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CALL cdiagh( nbase, hc, nvecx, ew, vc )
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!
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e(1:nvec) = ew(1:nvec)
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!
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END IF
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!
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! ... iterate
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!
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iterate: DO kter = 1, maxter
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!
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dav_iter = kter
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!
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CALL start_clock( 'update' )
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!
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np = 0
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!
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DO n = 1, nvec
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!
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IF ( .NOT. conv(n) ) THEN
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!
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! ... this root not yet converged ...
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!
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np = np + 1
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!
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! ... reorder eigenvectors so that coefficients for unconverged
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! ... roots come first. This allows to use quick matrix-matrix
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! ... multiplications to set a new basis vector (see below)
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!
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IF ( np /= n ) vc(:,np) = vc(:,n)
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!
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! ... for use in g_psi
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!
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ew(nbase+np) = e(n)
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!
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END IF
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!
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END DO
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!
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nb1 = nbase + 1
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!
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! ... expand the basis set with new basis vectors ( H - e*S )|psi> ...
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!
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CALL ZGEMM( 'N', 'N', kdim, notcnv, nbase, ONE, &
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spsi, kdmx, vc, nvecx, ZERO, psi(1,1,nb1), kdmx )
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!
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DO np = 1, notcnv
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!
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psi(:,:,nbase+np) = - ew(nbase+np)*psi(:,:,nbase+np)
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!
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END DO
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!
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CALL ZGEMM( 'N', 'N', kdim, notcnv, nbase, ONE, &
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hpsi, kdmx, vc, nvecx, ONE, psi(1,1,nb1), kdmx )
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!
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CALL stop_clock( 'update' )
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!
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! ... approximate inverse iteration
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!
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IF ( noncolin ) THEN
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!
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CALL g_psi_nc( ndmx, ndim, notcnv, npol, psi(1,1,nb1), ew(nb1) )
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!
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ELSE
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!
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CALL g_psi( ndmx, ndim, notcnv, psi(1,1,nb1), ew(nb1) )
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!
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END IF
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!
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! ... "normalize" correction vectors psi(:,nb1:nbase+notcnv) in
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! ... order to improve numerical stability of subspace diagonalization
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! ... (cdiagh) ew is used as work array :
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!
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! ... ew = <psi_i|psi_i>, i = nbase + 1, nbase + notcnv
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!
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DO n = 1, notcnv
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!
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nbn = nbase + n
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!
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IF ( npol == 1 ) THEN
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!
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ew(n) = DDOT( 2*ndim, psi(1,1,nbn), 1, psi(1,1,nbn), 1 )
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!
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ELSE
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!
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ew(n) = DDOT( 2*ndim, psi(1,1,nbn), 1, psi(1,1,nbn), 1 ) + &
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DDOT( 2*ndim, psi(1,2,nbn), 1, psi(1,2,nbn), 1 )
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!
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END IF
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!
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END DO
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!
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CALL reduce( notcnv, ew )
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!
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DO n = 1, notcnv
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!
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psi(:,:,nbase+n) = psi(:,:,nbase+n) / SQRT( ew(n) )
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!
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END DO
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!
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! ... here compute the hpsi and spsi of the new functions
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!
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IF ( noncolin ) THEN
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!
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CALL h_psi_nc( ndmx, ndim, notcnv, psi(1,1,nb1), hpsi(1,1,nb1) )
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!
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IF ( lelfield ) &
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CALL h_epsi_her( ndmx, ndim, &
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notcnv, psi(1,1,nb1), hpsi(1,1,nb1) )
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!
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IF ( uspp ) THEN
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!
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CALL s_psi_nc( ndmx, ndim, notcnv, psi(1,1,nb1), spsi(1,1,nb1) )
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!
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ELSE
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!
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spsi(:,:,nb1:nbase+notcnv) = psi(:,:,nb1:nbase+notcnv)
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!
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END IF
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!
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CALL cgramg1_nc( ndmx, nvecx, ndim, nb1, &
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nbase+notcnv, psi, spsi, hpsi, npol )
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!
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ELSE
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!
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CALL h_psi( ndmx, ndim, notcnv, psi(1,1,nb1), hpsi(1,1,nb1) )
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!
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IF ( lelfield ) &
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CALL h_epsi_her( ndmx, ndim, &
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notcnv, psi(1,1,nb1), hpsi(1,1,nb1) )
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!
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IF ( uspp ) THEN
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!
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CALL s_psi( ndmx, ndim, notcnv, psi(1,1,nb1), spsi(1,1,nb1) )
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!
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ELSE
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!
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spsi(:,:,nb1:nbase+notcnv) = psi(:,:,nb1:nbase+notcnv)
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!
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END IF
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!
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CALL cgramg1( kdmx, nvecx, kdim, &
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nb1, nbase+notcnv, psi, spsi, hpsi )
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!
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END IF
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!
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! ... update the reduced hamiltonian
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!
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CALL start_clock( 'uspp' )
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!
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CALL ZGEMM( 'C', 'N', nbase+notcnv, notcnv, kdim, ONE, psi, &
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kdmx, hpsi(1,1,nb1), kdmx, ZERO, hc(1,nb1), nvecx )
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!
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CALL reduce( 2*nvecx*notcnv, hc(1,nb1) )
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!
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CALL stop_clock( 'uspp' )
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!
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nbase = nbase + notcnv
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!
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DO n = 1, nbase
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!
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! ... the diagonal of hc must be strictly real
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!
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hc(n,n) = CMPLX( REAL( hc(n,n) ), 0.D0 )
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!
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DO m = n + 1, nbase
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!
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hc(m,n) = CONJG( hc(n,m) )
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!
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END DO
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!
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END DO
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!
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! ... diagonalize the reduced hamiltonian
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!
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CALL cdiagh( nbase, hc, nvecx, ew, vc )
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!
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! ... test for convergence
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!
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WHERE( btype(1:nvec) == 1 )
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!
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conv(1:nvec) = ( ( ABS( ew(1:nvec) - e(1:nvec) ) < ethr ) )
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!
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ELSEWHERE
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!
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conv(1:nvec) = ( ( ABS( ew(1:nvec) - e(1:nvec) ) < empty_ethr ) )
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!
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END WHERE
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!
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notcnv = COUNT( .NOT. conv(:) )
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!
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e(1:nvec) = ew(1:nvec)
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!
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! ... if overall convergence has been achieved, or the dimension of
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! ... the reduced basis set is becoming too large, or in any case if
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! ... we are at the last iteration refresh the basis set. i.e. replace
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! ... the first nvec elements with the current estimate of the
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! ... eigenvectors; set the basis dimension to nvec.
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!
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IF ( notcnv == 0 .OR. &
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nbase+notcnv > nvecx .OR. dav_iter == maxter ) THEN
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!
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CALL start_clock( 'last' )
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!
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CALL ZGEMM( 'N', 'N', kdim, nvec, nbase, ONE, &
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psi, kdmx, vc, nvecx, ZERO, evc, kdmx )
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!
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IF ( notcnv == 0 ) THEN
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!
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! ... all roots converged: return
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!
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CALL stop_clock( 'last' )
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!
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EXIT iterate
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!
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ELSE IF ( dav_iter == maxter ) THEN
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!
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! ... last iteration, some roots not converged: return
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!
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WRITE( stdout, '(5X,"WARNING: ",I5, &
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& " eigenvalues not converged")' ) notcnv
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!
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CALL stop_clock( 'last' )
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!
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EXIT iterate
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!
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END IF
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!
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! ... refresh psi, H*psi and S*psi
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!
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psi(:,:,1:nvec) = evc(:,:,1:nvec)
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!
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CALL ZGEMM( 'N', 'N', kdim, nvec, nbase, ONE, spsi, &
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kdmx, vc, nvecx, ZERO, psi(1,1,nvec+1), kdmx )
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!
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spsi(:,:,1:nvec) = psi(:,:,nvec+1:nvec+nvec)
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!
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CALL ZGEMM( 'N', 'N', kdim, nvec, nbase, ONE, hpsi, &
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kdmx, vc, nvecx, ZERO, psi(1,1,nvec+1), kdmx )
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!
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hpsi(:,:,1:nvec) = psi(:,:,nvec+1:nvec+nvec)
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!
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! ... refresh the reduced hamiltonian
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!
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nbase = nvec
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!
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hc(:,1:nbase) = ZERO
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vc(:,1:nbase) = ZERO
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!
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DO n = 1, nbase
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!
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hc(n,n) = REAL( e(n) )
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!
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vc(n,n) = ONE
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!
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END DO
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!
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CALL stop_clock( 'last' )
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!
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END IF
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!
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END DO iterate
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!
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DEALLOCATE( conv )
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DEALLOCATE( ew )
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DEALLOCATE( vc )
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DEALLOCATE( hc )
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DEALLOCATE( spsi )
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DEALLOCATE( hpsi )
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DEALLOCATE( psi )
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!
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END SUBROUTINE cegterg_para
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!
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!------------------------------------------------------------------------
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SUBROUTINE cegterg_serial()
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!------------------------------------------------------------------------
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!
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|
IMPLICIT NONE
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!
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|
ALLOCATE( psi( ndmx, npol, nvecx ) )
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|
ALLOCATE( hpsi( ndmx, npol, nvecx ) )
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!
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IF ( uspp ) ALLOCATE( spsi( ndmx, npol, nvecx ) )
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!
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ALLOCATE( sc( nvecx, nvecx ) )
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ALLOCATE( hc( nvecx, nvecx ) )
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ALLOCATE( vc( nvecx, nvecx ) )
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ALLOCATE( ew( nvecx ) )
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ALLOCATE( conv( nvec ) )
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!
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|
notcnv = nvec
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nbase = nvec
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conv = .FALSE.
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!
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IF ( uspp ) spsi = ZERO
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!
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|
hpsi = ZERO
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psi = ZERO
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psi(:,:,1:nvec) = evc(:,:,1:nvec)
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!
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! ... hpsi contains h times the basis vectors
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!
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IF ( noncolin ) THEN
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!
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CALL h_psi_nc( ndmx, ndim, nvec, psi, hpsi )
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!
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IF ( lelfield ) CALL h_epsi_her( ndmx, ndim, nvec, psi, hpsi )
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IF ( uspp ) CALL s_psi_nc( ndmx, ndim, nvec, psi, spsi )
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!
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|
ELSE
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!
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|
CALL h_psi( ndmx, ndim, nvec, psi, hpsi )
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!
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|
IF ( lelfield ) CALL h_epsi_her( ndmx, ndim, nvec, psi, hpsi )
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IF ( uspp ) CALL s_psi( ndmx, ndim, nvec, psi, spsi )
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!
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|
END IF
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|
!
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|
! ... hc contains the projection of the hamiltonian onto the reduced
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! ... space vc contains the eigenvectors of hc
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|
!
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|
hc(:,:) = ZERO
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sc(:,:) = ZERO
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vc(:,:) = ZERO
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!
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CALL ZGEMM( 'C', 'N', nbase, nbase, kdim, ONE, &
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|
psi, kdmx, hpsi, kdmx, ZERO, hc, nvecx )
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!
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CALL reduce( 2*nbase*nvecx, hc )
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!
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|
IF ( uspp ) THEN
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!
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|
CALL ZGEMM( 'C', 'N', nbase, nbase, kdim, ONE, &
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psi, kdmx, spsi, kdmx, ZERO, sc, nvecx )
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!
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|
ELSE
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!
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CALL ZGEMM( 'C', 'N', nbase, nbase, kdim, ONE, &
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|
psi, kdmx, psi, kdmx, ZERO, sc, nvecx )
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!
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|
END IF
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!
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|
CALL reduce( 2*nbase*nvecx, sc )
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!
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|
IF ( lrot ) THEN
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!
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DO n = 1, nbase
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!
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|
e(n) = REAL( hc(n,n) )
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!
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vc(n,n) = ONE
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!
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END DO
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!
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ELSE
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!
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! ... diagonalize the reduced hamiltonian
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!
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CALL cdiaghg( nbase, nvec, hc, sc, nvecx, ew, vc )
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!
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|
e(1:nvec) = ew(1:nvec)
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!
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END IF
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!
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|
! ... iterate
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!
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iterate: DO kter = 1, maxter
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!
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|
dav_iter = kter
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!
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|
CALL start_clock( 'update' )
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!
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|
np = 0
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|
!
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|
DO n = 1, nvec
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|
!
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|
IF ( .NOT. conv(n) ) THEN
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|
!
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|
! ... this root not yet converged ...
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|
!
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|
np = np + 1
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|
!
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|
! ... reorder eigenvectors so that coefficients for unconverged
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|
! ... roots come first. This allows to use quick matrix-matrix
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|
! ... multiplications to set a new basis vector (see below)
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|
!
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|
IF ( np /= n ) vc(:,np) = vc(:,n)
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|
!
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|
! ... for use in g_psi
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|
!
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|
ew(nbase+np) = e(n)
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|
!
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|
END IF
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|
!
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|
END DO
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|
!
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|
nb1 = nbase + 1
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|
!
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|
! ... expand the basis set with new basis vectors ( H - e*S )|psi> ...
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|
!
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|
IF ( uspp ) THEN
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|
!
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|
CALL ZGEMM( 'N', 'N', kdim, notcnv, nbase, ONE, spsi, &
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|
kdmx, vc, nvecx, ZERO, psi(1,1,nb1), kdmx )
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|
!
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|
ELSE
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|
!
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|
CALL ZGEMM( 'N', 'N', kdim, notcnv, nbase, ONE, psi, &
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|
kdmx, vc, nvecx, ZERO, psi(1,1,nb1), kdmx )
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|
!
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|
END IF
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|
!
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|
DO np = 1, notcnv
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|
!
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|
psi(:,:,nbase+np) = - ew(nbase+np)*psi(:,:,nbase+np)
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|
!
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|
END DO
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|
!
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|
CALL ZGEMM( 'N', 'N', kdim, notcnv, nbase, ONE, hpsi, &
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|
kdmx, vc, nvecx, ONE, psi(1,1,nb1), kdmx )
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|
!
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|
CALL stop_clock( 'update' )
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|
!
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|
! ... approximate inverse iteration
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|
!
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|
IF ( noncolin ) THEN
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|
!
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|
CALL g_psi_nc( ndmx, ndim, notcnv, npol, psi(1,1,nb1), ew(nb1) )
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|
!
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|
ELSE
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|
!
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|
CALL g_psi( ndmx, ndim, notcnv, psi(1,1,nb1), ew(nb1) )
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|
!
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|
END IF
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|
!
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|
! ... "normalize" correction vectors psi(:,nb1:nbase+notcnv) in
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|
! ... order to improve numerical stability of subspace diagonalization
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|
! ... (cdiaghg) ew is used as work array :
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|
!
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|
! ... ew = <psi_i|psi_i>, i = nbase + 1, nbase + notcnv
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|
!
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|
DO n = 1, notcnv
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|
!
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|
nbn = nbase + n
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|
!
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|
IF ( npol == 1 ) THEN
|
|
!
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|
ew(n) = DDOT( 2*ndim, psi(1,1,nbn), 1, psi(1,1,nbn), 1 )
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|
!
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|
ELSE
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|
!
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|
ew(n) = DDOT( 2*ndim, psi(1,1,nbn), 1, psi(1,1,nbn), 1 ) + &
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|
DDOT( 2*ndim, psi(1,2,nbn), 1, psi(1,2,nbn), 1 )
|
|
!
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|
END IF
|
|
!
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|
END DO
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|
!
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|
CALL reduce( notcnv, ew )
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|
!
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|
DO n = 1, notcnv
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|
!
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|
psi(:,:,nbase+n) = psi(:,:,nbase+n) / SQRT( ew(n) )
|
|
!
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|
END DO
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|
!
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|
! ... here compute the hpsi and spsi of the new functions
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|
!
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|
IF ( noncolin ) THEN
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|
!
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|
CALL h_psi_nc( ndmx, ndim, notcnv, psi(1,1,nb1), hpsi(1,1,nb1) )
|
|
!
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|
IF ( lelfield ) &
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|
CALL h_epsi_her( ndmx, ndim, &
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|
notcnv, psi(1,1,nb1), hpsi(1,1,nb1) )
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|
!
|
|
IF ( uspp ) &
|
|
CALL s_psi_nc( ndmx, ndim, notcnv, psi(1,1,nb1), spsi(1,1,nb1) )
|
|
!
|
|
ELSE
|
|
!
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|
CALL h_psi( ndmx, ndim, notcnv, psi(1,1,nb1), hpsi(1,1,nb1) )
|
|
!
|
|
IF ( lelfield ) &
|
|
CALL h_epsi_her( ndmx, ndim, &
|
|
notcnv, psi(1,1,nb1), hpsi(1,1,nb1) )
|
|
!
|
|
IF ( uspp ) &
|
|
CALL s_psi( ndmx, ndim, notcnv, psi(1,1,nb1), spsi(1,1,nb1) )
|
|
!
|
|
END IF
|
|
!
|
|
! ... update the reduced hamiltonian
|
|
!
|
|
CALL start_clock( 'uspp' )
|
|
!
|
|
CALL ZGEMM( 'C', 'N', nbase+notcnv, notcnv, kdim, ONE, psi, &
|
|
kdmx, hpsi(1,1,nb1), kdmx, ZERO, hc(1,nb1), nvecx )
|
|
!
|
|
CALL reduce( 2*nvecx*notcnv, hc(1,nb1) )
|
|
!
|
|
IF ( uspp ) THEN
|
|
!
|
|
CALL ZGEMM( 'C', 'N', nbase+notcnv, notcnv, kdim, ONE, psi, &
|
|
kdmx, spsi(1,1,nb1), kdmx, ZERO, sc(1,nb1), nvecx )
|
|
!
|
|
ELSE
|
|
!
|
|
CALL ZGEMM( 'C', 'N', nbase+notcnv, notcnv, kdim, ONE, psi, &
|
|
kdmx, psi(1,1,nb1), kdmx, ZERO, sc(1,nb1), nvecx )
|
|
!
|
|
END IF
|
|
!
|
|
CALL reduce( 2*nvecx*notcnv, sc(1,nb1) )
|
|
!
|
|
CALL stop_clock( 'uspp' )
|
|
!
|
|
nbase = nbase + notcnv
|
|
!
|
|
DO n = 1, nbase
|
|
!
|
|
! ... the diagonal of hc and sc must be strictly real
|
|
!
|
|
hc(n,n) = CMPLX( REAL( hc(n,n) ), 0.D0 )
|
|
sc(n,n) = CMPLX( REAL( sc(n,n) ), 0.D0 )
|
|
!
|
|
DO m = n + 1, nbase
|
|
!
|
|
hc(m,n) = CONJG( hc(n,m) )
|
|
sc(m,n) = CONJG( sc(n,m) )
|
|
!
|
|
END DO
|
|
!
|
|
END DO
|
|
!
|
|
! ... diagonalize the reduced hamiltonian
|
|
!
|
|
CALL cdiaghg( nbase, nvec, hc, sc, nvecx, ew, vc )
|
|
!
|
|
! ... test for convergence
|
|
!
|
|
WHERE( btype(1:nvec) == 1 )
|
|
!
|
|
conv(1:nvec) = ( ( ABS( ew(1:nvec) - e(1:nvec) ) < ethr ) )
|
|
!
|
|
ELSEWHERE
|
|
!
|
|
conv(1:nvec) = ( ( ABS( ew(1:nvec) - e(1:nvec) ) < empty_ethr ) )
|
|
!
|
|
END WHERE
|
|
!
|
|
notcnv = COUNT( .NOT. conv(:) )
|
|
!
|
|
e(1:nvec) = ew(1:nvec)
|
|
!
|
|
! ... if overall convergence has been achieved, or the dimension of
|
|
! ... the reduced basis set is becoming too large, or in any case if
|
|
! ... we are at the last iteration refresh the basis set. i.e. replace
|
|
! ... the first nvec elements with the current estimate of the
|
|
! ... eigenvectors; set the basis dimension to nvec.
|
|
!
|
|
IF ( notcnv == 0 .OR. &
|
|
nbase+notcnv > nvecx .OR. dav_iter == maxter ) THEN
|
|
!
|
|
CALL start_clock( 'last' )
|
|
!
|
|
CALL ZGEMM( 'N', 'N', kdim, nvec, nbase, ONE, &
|
|
psi, kdmx, vc, nvecx, ZERO, evc, kdmx )
|
|
!
|
|
IF ( notcnv == 0 ) THEN
|
|
!
|
|
! ... all roots converged: return
|
|
!
|
|
CALL stop_clock( 'last' )
|
|
!
|
|
EXIT iterate
|
|
!
|
|
ELSE IF ( dav_iter == maxter ) THEN
|
|
!
|
|
! ... last iteration, some roots not converged: return
|
|
!
|
|
WRITE( stdout, '(5X,"WARNING: ",I5, &
|
|
& " eigenvalues not converged")' ) notcnv
|
|
!
|
|
CALL stop_clock( 'last' )
|
|
!
|
|
EXIT iterate
|
|
!
|
|
END IF
|
|
!
|
|
! ... refresh psi, H*psi and S*psi
|
|
!
|
|
psi(:,:,1:nvec) = evc(:,:,1:nvec)
|
|
!
|
|
IF ( uspp ) THEN
|
|
!
|
|
CALL ZGEMM( 'N', 'N', kdim, nvec, nbase, ONE, spsi, &
|
|
kdmx, vc, nvecx, ZERO, psi(1,1,nvec+1), kdmx )
|
|
!
|
|
spsi(:,:,1:nvec) = psi(:,:,nvec+1:nvec+nvec)
|
|
!
|
|
END IF
|
|
!
|
|
CALL ZGEMM( 'N', 'N', kdim, nvec, nbase, ONE, hpsi, &
|
|
kdmx, vc, nvecx, ZERO, psi(1,1,nvec+1), kdmx )
|
|
!
|
|
hpsi(:,:,1:nvec) = psi(:,:,nvec+1:nvec+nvec)
|
|
!
|
|
! ... refresh the reduced hamiltonian
|
|
!
|
|
nbase = nvec
|
|
!
|
|
hc(:,1:nbase) = ZERO
|
|
sc(:,1:nbase) = ZERO
|
|
vc(:,1:nbase) = ZERO
|
|
!
|
|
DO n = 1, nbase
|
|
!
|
|
hc(n,n) = REAL( e(n) )
|
|
!
|
|
sc(n,n) = ONE
|
|
vc(n,n) = ONE
|
|
!
|
|
END DO
|
|
!
|
|
CALL stop_clock( 'last' )
|
|
!
|
|
END IF
|
|
!
|
|
END DO iterate
|
|
!
|
|
DEALLOCATE( conv )
|
|
DEALLOCATE( ew )
|
|
DEALLOCATE( vc )
|
|
DEALLOCATE( hc )
|
|
DEALLOCATE( sc )
|
|
!
|
|
IF ( uspp ) DEALLOCATE( spsi )
|
|
!
|
|
DEALLOCATE( hpsi )
|
|
DEALLOCATE( psi )
|
|
!
|
|
END SUBROUTINE cegterg_serial
|
|
!
|
|
END SUBROUTINE cegterg
|