quantum-espresso/PH/find_mode_sym.f90

228 lines
6.3 KiB
Fortran

!
! Copyright (C) 2006 Quantum-ESPRESSO 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 .
!
SUBROUTINE find_mode_sym (dyn, w2, at, bg, nat, nsym, s, irt, xq, rtau, &
amass, ntyp, ityp)
!
! This subroutine finds the irreducible representations which give
! the transformation properties of eigenvectors of the dynamical
! matrix. It does NOT work at zone border in non symmorphic space groups.
!
!
#include "f_defs.h"
USE io_global, ONLY : stdout
USE kinds, ONLY : DP
USE noncollin_module, ONLY : noncolin
USE spin_orb, ONLY : domag
USE ions_base, ONLY : tau
USE rap_point_group, ONLY : code_group, nclass, nelem, elem, which_irr, &
char_mat, name_rap, name_class, gname, ir_ram
USE rap_point_group_is, ONLY : gname_is
USE control_ph, ONLY : lgamma, lgamma_gamma
IMPLICIT NONE
INTEGER :: &
nat, nsym, &
ntyp, ityp(nat), &
irt(48,nat), &
s(3,3,48)
REAL(DP) :: &
at(3,3), &
bg(3,3), &
xq(3), &
rtau(3,48,nat), &
amass(ntyp), &
w2(3*nat)
COMPLEX(DP) :: &
dyn(3*nat, 3*nat)
REAL(DP), PARAMETER :: eps=1.d-5, &
rydcm1 = 13.6058d0 * 8065.5d0
INTEGER :: &
ngroup, & ! number of different frequencies groups
nmodes, & ! number of modes
imode, imode1, igroup, dim_rap, nu_i, nu_j, &
irot, irap, iclass, mu, na, i, j
INTEGER, ALLOCATABLE :: istart(:)
REAL(DP) :: sr(3,3,48)
COMPLEX(DP) :: ZDOTC, times ! safe dimension
! in case of accidental degeneracy
REAL(DP), ALLOCATABLE :: w1(:)
COMPLEX(DP), ALLOCATABLE :: rmode(:), trace(:,:), z(:,:)
LOGICAL :: is_linear
CHARACTER(3) :: cdum
!
! Divide the modes on the basis of the mode degeneracy.
!
nmodes=3*nat
ALLOCATE(istart(nmodes+1))
ALLOCATE(z(nmodes,nmodes))
ALLOCATE(w1(nmodes))
ALLOCATE(rmode(nmodes))
ALLOCATE(trace(48,nmodes))
DO nu_i = 1, nmodes
DO mu = 1, nmodes
na = (mu - 1) / 3 + 1
z (mu, nu_i) = dyn (mu, nu_i) * SQRT (amass (ityp (na) ) )
END DO
END DO
DO imode=1,nmodes
w1(imode)=SIGN(SQRT(ABS(w2(imode)))*rydcm1,w2(imode))
ENDDO
DO irot=1,nsym
CALL s_axis_to_cart (s(1,1,irot), sr(1,1,irot), at, bg)
END DO
ngroup=1
istart(ngroup)=1
imode1=1
IF (lgamma_gamma) THEN
istart(ngroup)=7
imode1=6
IF(is_linear(nat,tau)) istart(ngroup)=6
ENDIF
DO imode=imode1+1,nmodes
IF (ABS(w1(imode)-w1(imode-1)) > 5.0d-2) THEN
ngroup=ngroup+1
istart(ngroup)=imode
END IF
END DO
istart(ngroup+1)=nmodes+1
!
! Find the character of one symmetry operation per class
!
DO igroup=1,ngroup
dim_rap=istart(igroup+1)-istart(igroup)
DO iclass=1,nclass
irot=elem(1,iclass)
trace(iclass,igroup)=(0.d0,0.d0)
DO i=1,dim_rap
nu_i=istart(igroup)+i-1
CALL rotate_mod(z(1,nu_i),rmode,sr(1,1,irot),irt,rtau,xq,nat,irot)
trace(iclass,igroup)=trace(iclass,igroup) + &
ZDOTC(3*nat,z(1,nu_i),1,rmode,1)
END DO
! write(6,*) igroup,iclass, trace(iclass,igroup)
END DO
END DO
!
! And now use the character table to identify the symmetry representation
! of each group of modes
!
IF (noncolin.and.domag) THEN
WRITE(stdout, &
'(/,5x,"Mode symmetry, ",a11," [",a11,"] magnetic point group:",/)') &
gname, gname_is
ELSE
WRITE(stdout,'(/,5x,"Mode symmetry, ",a11," point group:",/)') gname
END IF
DO igroup=1,ngroup
DO irap=1,nclass
times=(0.d0,0.d0)
DO iclass=1,nclass
times=times+CONJG(trace(iclass,igroup))*char_mat(irap, &
which_irr(iclass))*nelem(iclass)
! write(6,*) igroup, irap, iclass, which_irr(iclass)
ENDDO
times=times/nsym
cdum=" "
IF (lgamma) cdum=ir_ram(irap)
IF ((ABS(NINT(DBLE(times))-DBLE(times)) > 1.d-4).OR. &
(ABS(AIMAG(times)) > eps) ) THEN
WRITE(stdout,'(5x,"omega(",i3," -",i3,") = ",f12.1,2x,"[cm-1]",3x, "--> ?")') &
istart(igroup), istart(igroup+1)-1, w1(istart(igroup))
ENDIF
IF (ABS(times) > eps) THEN
IF (ABS(NINT(DBLE(times))-1.d0) < 1.d-4) THEN
WRITE(stdout,'(5x, "omega(",i3," -",i3,") = ",f12.1,2x,"[cm-1]",3x,"--> ",a19)') &
istart(igroup), istart(igroup+1)-1, w1(istart(igroup)), &
name_rap(irap)//" "//cdum
ELSE
WRITE(stdout,'(5x,"omega(",i3," -",i3,") = ",f12.1,2x,"[cm-1]",3x,"--> ",i3,a19)') &
istart(igroup), istart(igroup+1)-1, &
w1(istart(igroup)), NINT(DBLE(times)), &
name_rap(irap)//" "//cdum
END IF
END IF
END DO
END DO
WRITE( stdout, '(/,1x,74("*"))')
DEALLOCATE(trace)
DEALLOCATE(z)
DEALLOCATE(w1)
DEALLOCATE(rmode)
DEALLOCATE(istart)
RETURN
END SUBROUTINE find_mode_sym
SUBROUTINE rotate_mod(mode,rmode,sr,irt,rtau,xq,nat,irot)
USE kinds, ONLY : DP
USE constants, ONLY: tpi
IMPLICIT NONE
INTEGER :: nat, irot, irt(48,nat)
COMPLEX(DP) :: mode(3*nat), rmode(3*nat), phase
REAL(DP) :: sr(3,3), rtau(3,48,nat), xq(3), arg
INTEGER :: na, nb, ipol, kpol, mu_i, mu_k
rmode=(0.d0,0.d0)
DO na=1,nat
nb=irt(irot,na)
arg = ( xq(1)*rtau(1,irot,na) + xq(2)*rtau(2,irot,na)+ &
xq(3)*rtau(3,irot,na) ) * tpi
phase = cmplx(cos(arg), sin(arg))
DO ipol=1,3
mu_i=3*(na-1)+ipol
DO kpol=1,3
mu_k=3*(nb-1)+kpol
rmode(mu_i)=rmode(mu_i) + sr(kpol,ipol)*mode(mu_k)*phase
END DO
END DO
END DO
RETURN
END SUBROUTINE rotate_mod
FUNCTION is_linear(nat,tau)
!
! This function is true if the nat atoms are all on the same line
!
USE kinds, ONLY : DP
IMPLICIT NONE
LOGICAL :: is_linear
INTEGER, INTENT(IN) :: nat
REAL(DP), INTENT(IN) :: tau(3,nat)
REAL(DP) :: u(3), v(3), umod, vmod
INTEGER :: na
is_linear=.TRUE.
IF (nat<=2) RETURN
u(:)=tau(:,2)-tau(:,1)
umod=sqrt(u(1)**2+u(2)**2+u(3)**2)
DO na=3,nat
v(:)=tau(:,na)-tau(:,1)
vmod=sqrt(v(1)**2+v(2)**2+v(3)**2)
is_linear=is_linear.AND.(abs(1.0_DP- &
abs(u(1)*v(1)+u(2)*v(2)+u(3)*v(3))/umod/vmod)<1.d-4)
ENDDO
RETURN
END