quantum-espresso/PH/sym_def.f90

73 lines
1.9 KiB
Fortran

!
! Copyright (C) 2001 PWSCF group
! This file is distributed under the terms of the
! GNU General Public License. See the file `License'
! in the root directory of the present distribution,
! or http://www.gnu.org/copyleft/gpl.txt .
!
#include "f_defs.h"
!---------------------------------------------------------------------
subroutine sym_def (def, irr)
!---------------------------------------------------------------------
! Symmetrizes the first order changes of the Fermi energies of an
! irreducible representation. These objects are defined complex because
! perturbations may be complex
!
! Used in the q=0 metallic case only.
!
USE kinds, only : DP
use phcom
implicit none
integer :: irr
! input: the representation under consideration
complex(DP) :: def (npertx)
! inp/out: the fermi energy changes
integer :: ipert, jpert, isym, irot
! counter on perturbations
! counter on perturbations
! counter on symmetries
! the rotation
complex(DP) :: w_def (npertx)
! the fermi energy changes (work array)
if (nsymq == 1 .and. (.not.minus_q) ) return
!
! first the symmetrization S(irotmq)*q = -q + Gi if necessary
!
if (minus_q) then
w_def = (0.d0, 0.d0)
do ipert = 1, npert (irr)
do jpert = 1, npert (irr)
w_def (ipert) = w_def (ipert) + tmq (jpert, ipert, irr) &
* def (jpert)
enddo
enddo
do ipert = 1, npert (irr)
def (ipert) = 0.5d0 * (def (ipert) + CONJG(w_def (ipert) ) )
enddo
endif
!
! Here we symmetrize with respect to the small group of q
!
w_def = (0.d0, 0.d0)
do ipert = 1, npert (irr)
do isym = 1, nsymq
irot = irgq (isym)
do jpert = 1, npert (irr)
w_def (ipert) = w_def (ipert) + t (jpert, ipert, irot, irr) &
* def (jpert)
enddo
enddo
enddo
!
! normalize and exit
!
def = w_def / DBLE(nsymq)
return
end subroutine sym_def