mirror of https://gitlab.com/QEF/q-e.git
3049 lines
95 KiB
Fortran
3049 lines
95 KiB
Fortran
!
|
|
! Copyright (C) 2002-2005 FPMD-CPV groups
|
|
! 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 atomic_wfc(eigr,n_atomic_wfc,wfc)
|
|
!-----------------------------------------------------------------------
|
|
!
|
|
! Compute atomic wavefunctions in G-space
|
|
!
|
|
USE gvecw, ONLY: ngw
|
|
USE reciprocal_vectors, ONLY: gstart, g, gx
|
|
USE ions_base, ONLY: nsp, na, nat
|
|
USE cell_base, ONLY: tpiba
|
|
USE atom, ONLY: nchi, lchi, mesh, r, chi, rab
|
|
!
|
|
IMPLICIT NONE
|
|
INTEGER, INTENT(in) :: n_atomic_wfc
|
|
COMPLEX(8), INTENT(in) :: eigr(ngw,nat)
|
|
COMPLEX(8), INTENT(out):: wfc(ngw,n_atomic_wfc)
|
|
!
|
|
INTEGER :: natwfc, ndm, is, ia, ir, nb, l, m, lm, i, lmax_wfc, isa
|
|
REAL(8), ALLOCATABLE:: ylm(:,:), q(:), jl(:), vchi(:), &
|
|
& chiq(:)
|
|
!
|
|
! calculate max angular momentum required in wavefunctions
|
|
!
|
|
lmax_wfc=-1
|
|
DO is = 1,nsp
|
|
DO nb = 1, nchi(is)
|
|
lmax_wfc = MAX (lmax_wfc, lchi (nb, is) )
|
|
ENDDO
|
|
ENDDO
|
|
ALLOCATE(ylm(ngw,(lmax_wfc+1)**2))
|
|
CALL ylmr2 ((lmax_wfc+1)**2, ngw, gx, g, ylm)
|
|
ndm = MAXVAL(mesh(1:nsp))
|
|
ALLOCATE(jl(ndm), vchi(ndm))
|
|
ALLOCATE(q(ngw), chiq(ngw))
|
|
!
|
|
DO i=1,ngw
|
|
q(i) = SQRT(g(i))*tpiba
|
|
END DO
|
|
!
|
|
natwfc=0
|
|
isa = 0
|
|
DO is=1,nsp
|
|
!
|
|
! radial fourier transform of the chi functions
|
|
! NOTA BENE: chi is r times the radial part of the atomic wavefunction
|
|
!
|
|
DO nb = 1,nchi(is)
|
|
l = lchi(nb,is)
|
|
DO i=1,ngw
|
|
CALL sph_bes (mesh(is), r(1,is), q(i), l, jl)
|
|
DO ir=1,mesh(is)
|
|
vchi(ir) = chi(ir,nb,is)*r(ir,is)*jl(ir)
|
|
ENDDO
|
|
CALL simpson_cp90(mesh(is),vchi,rab(1,is),chiq(i))
|
|
ENDDO
|
|
!
|
|
! multiply by angular part and structure factor
|
|
! NOTA BENE: the factor i^l MUST be present!!!
|
|
!
|
|
DO m = 1,2*l+1
|
|
lm = l**2 + m
|
|
DO ia = 1 + isa, na(is) + isa
|
|
natwfc = natwfc + 1
|
|
wfc(:,natwfc) = (0.d0,1.d0)**l * eigr(:,ia)* ylm(:,lm)*chiq(:)
|
|
ENDDO
|
|
ENDDO
|
|
ENDDO
|
|
isa = isa + na(is)
|
|
ENDDO
|
|
!
|
|
IF (natwfc.NE.n_atomic_wfc) &
|
|
& CALL errore('atomic_wfc','unexpected error',natwfc)
|
|
!
|
|
DEALLOCATE(q, chiq, vchi, jl, ylm)
|
|
!
|
|
RETURN
|
|
END SUBROUTINE atomic_wfc
|
|
!
|
|
!
|
|
|
|
!-----------------------------------------------------------------------
|
|
REAL(8) FUNCTION cscnorm( bec, nkbx, cp, ngwx, i, n )
|
|
!-----------------------------------------------------------------------
|
|
! requires in input the updated bec(i)
|
|
!
|
|
USE ions_base, ONLY: na
|
|
USE gvecw, ONLY: ngw
|
|
USE reciprocal_vectors, ONLY: gstart
|
|
USE cvan, ONLY: ish, nvb
|
|
USE uspp_param, ONLY: nh
|
|
USE uspp, ONLY: qq
|
|
USE mp, ONLY: mp_sum
|
|
USE mp_global, ONLY: intra_image_comm
|
|
USE kinds, ONLY: DP
|
|
!
|
|
IMPLICIT NONE
|
|
INTEGER, INTENT(IN) :: i, n
|
|
INTEGER, INTENT(IN) :: ngwx, nkbx
|
|
REAL(DP) :: bec( nkbx, n )
|
|
COMPLEX(DP) :: cp( ngwx, n )
|
|
!
|
|
INTEGER ig, is, iv, jv, ia, inl, jnl
|
|
REAL(8) rsum
|
|
REAL(8), ALLOCATABLE:: temp(:)
|
|
!
|
|
!
|
|
ALLOCATE(temp(ngw))
|
|
DO ig=1,ngw
|
|
temp(ig)=DBLE(CONJG(cp(ig,i))*cp(ig,i))
|
|
END DO
|
|
rsum=2.*SUM(temp)
|
|
IF (gstart == 2) rsum=rsum-temp(1)
|
|
|
|
CALL mp_sum( rsum, intra_image_comm )
|
|
|
|
DEALLOCATE(temp)
|
|
!
|
|
DO is=1,nvb
|
|
DO iv=1,nh(is)
|
|
DO jv=1,nh(is)
|
|
IF(ABS(qq(iv,jv,is)).GT.1.e-5) THEN
|
|
DO ia=1,na(is)
|
|
inl=ish(is)+(iv-1)*na(is)+ia
|
|
jnl=ish(is)+(jv-1)*na(is)+ia
|
|
rsum = rsum + &
|
|
& qq(iv,jv,is)*bec(inl,i)*bec(jnl,i)
|
|
END DO
|
|
ENDIF
|
|
END DO
|
|
END DO
|
|
END DO
|
|
!
|
|
cscnorm=SQRT(rsum)
|
|
!
|
|
RETURN
|
|
END FUNCTION cscnorm
|
|
!
|
|
!-----------------------------------------------------------------------
|
|
SUBROUTINE denkin(c,dekin)
|
|
!-----------------------------------------------------------------------
|
|
!
|
|
USE constants, ONLY: pi, fpi
|
|
USE electrons_base, ONLY: n => nbsp, nx => nbspx, f
|
|
USE gvecw, ONLY: ngw
|
|
USE reciprocal_vectors, ONLY: gstart, g, gx
|
|
USE cell_base, ONLY: ainv, tpiba2
|
|
USE gvecw, ONLY: ggp, ecutz, ecsig, ecfix
|
|
USE mp, ONLY: mp_sum
|
|
USE mp_global, ONLY: intra_image_comm
|
|
!
|
|
IMPLICIT NONE
|
|
! input
|
|
COMPLEX(8) c(ngw,nx)
|
|
! output
|
|
REAL(8) dekin(3,3)
|
|
! local
|
|
INTEGER j, k, ig, i
|
|
REAL(8), ALLOCATABLE:: gtmp(:)
|
|
REAL(8) sk(n) ! automatic array
|
|
REAL(8) :: ga, dggp, efac
|
|
!
|
|
ALLOCATE (gtmp(ngw))
|
|
dekin=0.d0
|
|
DO j=1,3
|
|
DO k=1,3
|
|
DO ig=1,ngw
|
|
efac = 2.d0 * ecutz / ecsig / SQRT(pi)
|
|
dggp = 1.d0 + efac * EXP( - ( tpiba2 * g(ig) - ecfix ) * ( tpiba2 * g(ig) - ecfix ) / ecsig / ecsig )
|
|
ga = gx(1,ig) * ainv(k,1) + gx(2,ig) * ainv(k,2) + gx(3,ig) * ainv(k,3)
|
|
gtmp(ig) = gx(j,ig) * ga * dggp
|
|
END DO
|
|
DO i=1,n
|
|
sk(i)=0.d0
|
|
DO ig=gstart,ngw
|
|
sk(i)=sk(i)+DBLE(CONJG(c(ig,i))*c(ig,i))*gtmp(ig)
|
|
END DO
|
|
END DO
|
|
DO i=1,n
|
|
dekin(j,k)=dekin(j,k)-2.d0*tpiba2*(f(i)*sk(i))
|
|
END DO
|
|
END DO
|
|
END DO
|
|
DEALLOCATE (gtmp)
|
|
|
|
CALL mp_sum( dekin( 1:3, 1:3 ), intra_image_comm )
|
|
!
|
|
RETURN
|
|
END SUBROUTINE denkin
|
|
!
|
|
!-----------------------------------------------------------------------
|
|
SUBROUTINE denh(rhotmp,drhotmp,sfac,vtemp,eh,dh)
|
|
!-----------------------------------------------------------------------
|
|
!
|
|
! derivative of hartree energy wrt cell parameters h
|
|
! Output in dh
|
|
!
|
|
! rhotmp input : total electronic + ionic broadened charge (G)
|
|
! drhotmp input and work space
|
|
! sfac input : structure factors
|
|
! wtemp work space
|
|
! eh input: hartree energy
|
|
!
|
|
USE constants, ONLY: pi, fpi
|
|
USE ions_base, ONLY: nsp
|
|
USE gvecs
|
|
USE gvecp, ONLY: ng => ngm
|
|
USE reciprocal_vectors, ONLY: gstart, gx, g
|
|
USE cell_base, ONLY: omega
|
|
USE cell_base, ONLY: ainv, tpiba2
|
|
USE local_pseudo, ONLY: rhops, drhops
|
|
USE mp, ONLY: mp_sum
|
|
USE mp_global, ONLY: intra_image_comm
|
|
|
|
IMPLICIT NONE
|
|
! input
|
|
COMPLEX(8) rhotmp(ng), drhotmp(ng,3,3), vtemp(ng), sfac(ngs,nsp)
|
|
REAL(8) eh
|
|
! output
|
|
REAL(8) dh(3,3)
|
|
! local
|
|
INTEGER i, j, ig, is
|
|
REAL(8) wz
|
|
!
|
|
! wz = factor for g.neq.0 because of c*(g)=c(-g)
|
|
!
|
|
wz=2.d0
|
|
DO j=1,3
|
|
DO i=1,3
|
|
DO is=1,nsp
|
|
DO ig=1,ngs
|
|
drhotmp(ig,i,j) = drhotmp(ig,i,j) - &
|
|
& sfac(ig,is)*drhops(ig,is)* &
|
|
& 2.d0*tpiba2*gx(i,ig)*(gx(1,ig)*ainv(j,1)+ &
|
|
& gx(2,ig)*ainv(j,2)+gx(3,ig)*ainv(j,3))- &
|
|
& sfac(ig,is)*rhops(ig,is)*ainv(j,i)
|
|
ENDDO
|
|
ENDDO
|
|
IF (gstart == 2) vtemp(1)=(0.d0,0.d0)
|
|
DO ig=gstart,ng
|
|
vtemp(ig)=CONJG(rhotmp(ig))*rhotmp(ig)/(tpiba2*g(ig))**2 &
|
|
& * tpiba2*gx(i,ig)*(gx(1,ig)*ainv(j,1)+ &
|
|
& gx(2,ig)*ainv(j,2)+gx(3,ig)*ainv(j,3)) + &
|
|
& CONJG(rhotmp(ig))/(tpiba2*g(ig))*drhotmp(ig,i,j)
|
|
ENDDO
|
|
dh(i,j)=fpi*omega*DBLE(SUM(vtemp))*wz
|
|
ENDDO
|
|
ENDDO
|
|
|
|
CALL mp_sum( dh( 1:3, 1:3 ), intra_image_comm )
|
|
|
|
DO i=1,3
|
|
DO j=1,3
|
|
dh(i,j)=dh(i,j)+omega*eh*ainv(j,i)
|
|
END DO
|
|
END DO
|
|
|
|
RETURN
|
|
END SUBROUTINE denh
|
|
!
|
|
!-----------------------------------------------------------------------
|
|
SUBROUTINE denps(rhotmp,drhotmp,sfac,vtemp,dps)
|
|
!-----------------------------------------------------------------------
|
|
!
|
|
! derivative of local potential energy wrt cell parameters h
|
|
! Output in dps
|
|
!
|
|
! rhotmp input : rho(G) (up and down spin components summed)
|
|
! drhotmp input
|
|
! sfac input : structure factors
|
|
! wtemp work space
|
|
!
|
|
USE ions_base, ONLY: nsp
|
|
USE gvecs, ONLY: ngs
|
|
USE gvecp, ONLY: ng => ngm
|
|
USE reciprocal_vectors, ONLY: gstart, gx
|
|
USE cell_base, ONLY: omega
|
|
USE cell_base, ONLY: ainv, tpiba2
|
|
USE local_pseudo, ONLY: vps, dvps
|
|
USE mp, ONLY: mp_sum
|
|
USE mp_global, ONLY: intra_image_comm
|
|
|
|
IMPLICIT NONE
|
|
! input
|
|
COMPLEX(8) rhotmp(ng), drhotmp(ng,3,3), vtemp(ng), sfac(ngs,nsp)
|
|
! output
|
|
REAL(8) dps(3,3)
|
|
! local
|
|
INTEGER i, j, ig, is
|
|
REAL(8) wz
|
|
!
|
|
! wz = factor for g.neq.0 because of c*(g)=c(-g)
|
|
!
|
|
wz=2.d0
|
|
DO i=1,3
|
|
DO j=1,3
|
|
DO ig=1,ngs
|
|
vtemp(ig)=(0.,0.)
|
|
ENDDO
|
|
DO is=1,nsp
|
|
DO ig=1,ngs
|
|
vtemp(ig)=vtemp(ig)-CONJG(rhotmp(ig))*sfac(ig,is)* &
|
|
& dvps(ig,is)*2.d0*tpiba2*gx(i,ig)* &
|
|
& (gx(1,ig)*ainv(j,1) + &
|
|
& gx(2,ig)*ainv(j,2) + &
|
|
& gx(3,ig)*ainv(j,3) ) + &
|
|
& CONJG(drhotmp(ig,i,j))*sfac(ig,is)*vps(ig,is)
|
|
ENDDO
|
|
ENDDO
|
|
dps(i,j)=omega*DBLE(wz*SUM(vtemp))
|
|
IF (gstart == 2) dps(i,j)=dps(i,j)-omega*DBLE(vtemp(1))
|
|
ENDDO
|
|
ENDDO
|
|
|
|
CALL mp_sum( dps( 1:3, 1:3 ), intra_image_comm )
|
|
|
|
RETURN
|
|
END SUBROUTINE denps
|
|
|
|
|
|
!-----------------------------------------------------------------------
|
|
SUBROUTINE denlcc( nnr, nspin, vxcr, sfac, drhocg, dcc )
|
|
!-----------------------------------------------------------------------
|
|
!
|
|
! derivative of non linear core correction exchange energy wrt cell
|
|
! parameters h
|
|
! Output in dcc
|
|
!
|
|
USE kinds, ONLY: DP
|
|
USE ions_base, ONLY: nsp
|
|
USE reciprocal_vectors, ONLY: gstart, gx, ngs, g, ngm
|
|
USE recvecs_indexes, ONLY: np
|
|
USE cell_base, ONLY: omega, ainv, tpiba2
|
|
USE mp, ONLY: mp_sum
|
|
USE mp_global, ONLY: intra_image_comm
|
|
USE atom, ONLY: nlcc
|
|
USE grid_dimensions, ONLY: nr1, nr2, nr3, nr1x, nr2x, nr3x
|
|
USE fft_module, ONLY: fwfft
|
|
|
|
IMPLICIT NONE
|
|
|
|
! input
|
|
|
|
INTEGER, INTENT(IN) :: nnr, nspin
|
|
REAL(DP) :: vxcr( nnr, nspin )
|
|
COMPLEX(DP) :: sfac( ngs, nsp )
|
|
REAL(DP) :: drhocg( ngm, nsp )
|
|
|
|
! output
|
|
|
|
REAL(DP), INTENT(OUT) :: dcc(3,3)
|
|
|
|
! local
|
|
|
|
INTEGER :: i, j, ig, is
|
|
COMPLEX(DP) :: srhoc
|
|
REAL(DP) :: vxcc
|
|
!
|
|
COMPLEX(DP), ALLOCATABLE :: vxc( : )
|
|
!
|
|
dcc = 0.0d0
|
|
!
|
|
ALLOCATE( vxc( nnr ) )
|
|
!
|
|
vxc(:) = vxcr(:,1)
|
|
!
|
|
IF( nspin > 1 ) vxc(:) = vxc(:) + vxcr(:,2)
|
|
!
|
|
CALL fwfft( 'Dense', vxc, nr1, nr2, nr3, nr1x, nr2x, nr3x )
|
|
!
|
|
DO i=1,3
|
|
DO j=1,3
|
|
DO ig = gstart, ngs
|
|
srhoc = 0.0d0
|
|
DO is = 1, nsp
|
|
IF( nlcc( is ) ) srhoc = srhoc + sfac( ig, is ) * drhocg( ig, is )
|
|
ENDDO
|
|
vxcc = DBLE( CONJG( vxc( np( ig ) ) ) * srhoc ) / SQRT( g( ig ) * tpiba2 )
|
|
dcc(i,j) = dcc(i,j) + vxcc * &
|
|
& 2.d0 * tpiba2 * gx(i,ig) * &
|
|
& (gx(1,ig)*ainv(j,1) + &
|
|
& gx(2,ig)*ainv(j,2) + &
|
|
& gx(3,ig)*ainv(j,3) )
|
|
ENDDO
|
|
ENDDO
|
|
ENDDO
|
|
|
|
DEALLOCATE( vxc )
|
|
|
|
dcc = dcc * omega
|
|
|
|
CALL mp_sum( dcc( 1:3, 1:3 ), intra_image_comm )
|
|
|
|
RETURN
|
|
END SUBROUTINE denlcc
|
|
|
|
|
|
|
|
!
|
|
!-------------------------------------------------------------------------
|
|
SUBROUTINE dforce (bec,betae,i,c,ca,df,da,v)
|
|
!-----------------------------------------------------------------------
|
|
!computes: the generalized force df=CMPLX(dfr,dfi) acting on the i-th
|
|
! electron state at the gamma point of the brillouin zone
|
|
! represented by the vector c=CMPLX(cr,ci)
|
|
!
|
|
! d_n(g) = f_n { 0.5 g^2 c_n(g) + [vc_n](g) +
|
|
! sum_i,ij d^q_i,ij (-i)**l beta_i,i(g)
|
|
! e^-ig.r_i < beta_i,j | c_n >}
|
|
USE kinds, ONLY: dp
|
|
USE control_flags, ONLY: iprint, tbuff
|
|
USE gvecs
|
|
USE gvecw, ONLY: ngw
|
|
USE cvan, ONLY: ish
|
|
USE uspp, ONLY: nhsa=>nkb, dvan, deeq
|
|
USE uspp_param, ONLY: nhm, nh
|
|
USE smooth_grid_dimensions, ONLY: nr1s, nr2s, nr3s, &
|
|
nr1sx, nr2sx, nr3sx, nnrsx
|
|
USE electrons_base, ONLY: n => nbsp, ispin, f, nspin
|
|
USE constants, ONLY: pi, fpi
|
|
USE ions_base, ONLY: nsp, na, nat
|
|
USE gvecw, ONLY: ggp
|
|
USE cell_base, ONLY: tpiba2
|
|
USE ensemble_dft, ONLY: tens
|
|
USE funct, ONLY: dft_is_meta
|
|
USE fft_module, ONLY: fwfft, invfft
|
|
!
|
|
IMPLICIT NONE
|
|
!
|
|
COMPLEX(8) betae(ngw,nhsa), c(ngw), ca(ngw), df(ngw), da(ngw)
|
|
REAL(8) bec(nhsa,n), v(nnrsx,nspin)
|
|
INTEGER i
|
|
! local variables
|
|
INTEGER iv, jv, ia, is, isa, ism, ios, iss1, iss2, ir, ig, inl, jnl
|
|
REAL(8) fi, fip, dd
|
|
COMPLEX(8) fp,fm,ci
|
|
REAL(8) af(nhsa), aa(nhsa) ! automatic arrays
|
|
COMPLEX(8) dtemp(ngw) !
|
|
COMPLEX(8), ALLOCATABLE :: psi(:)
|
|
!
|
|
!
|
|
CALL start_clock( 'dforce' )
|
|
!
|
|
ALLOCATE( psi( nnrsx ) )
|
|
!
|
|
! important: if n is odd => c(*,n+1)=0.
|
|
!
|
|
IF (MOD(n,2).NE.0.AND.i.EQ.n) THEN
|
|
DO ig=1,ngw
|
|
ca(ig)=(0.,0.)
|
|
END DO
|
|
ENDIF
|
|
!
|
|
ci=(0.0,1.0)
|
|
!
|
|
IF (.NOT.tbuff) THEN
|
|
!
|
|
psi (:) = (0.d0, 0.d0)
|
|
DO ig=1,ngw
|
|
psi(nms(ig))=CONJG(c(ig)-ci*ca(ig))
|
|
psi(nps(ig))=c(ig)+ci*ca(ig)
|
|
END DO
|
|
!
|
|
CALL invfft('Wave',psi,nr1s,nr2s,nr3s,nr1sx,nr2sx,nr3sx)
|
|
!
|
|
ELSE
|
|
!
|
|
! read psi from buffer 21
|
|
!
|
|
READ(21,iostat=ios) psi
|
|
IF(ios.NE.0) CALL errore &
|
|
& (' dforce',' error in reading unit 21',ios)
|
|
!
|
|
ENDIF
|
|
!
|
|
iss1=ispin(i)
|
|
!
|
|
! the following avoids a potential out-of-bounds error
|
|
!
|
|
IF (i.NE.n) THEN
|
|
iss2=ispin(i+1)
|
|
ELSE
|
|
iss2=iss1
|
|
END IF
|
|
!
|
|
DO ir=1,nnrsx
|
|
psi(ir)=CMPLX(v(ir,iss1)* DBLE(psi(ir)), v(ir,iss2)*AIMAG(psi(ir)) )
|
|
END DO
|
|
!
|
|
CALL fwfft('Wave',psi,nr1s,nr2s,nr3s,nr1sx,nr2sx,nr3sx)
|
|
!
|
|
! note : the factor 0.5 appears
|
|
! in the kinetic energy because it is defined as 0.5*g**2
|
|
! in the potential part because of the logics
|
|
!
|
|
|
|
IF (tens) THEN
|
|
fi =-0.5
|
|
fip=-0.5
|
|
ELSE
|
|
fi =- f(i)*0.5
|
|
fip=-f(i+1)*0.5
|
|
END IF
|
|
|
|
DO ig=1,ngw
|
|
fp= psi(nps(ig)) + psi(nms(ig))
|
|
fm= psi(nps(ig)) - psi(nms(ig))
|
|
df(ig)= fi*(tpiba2*ggp(ig)* c(ig)+CMPLX(DBLE(fp), AIMAG(fm)))
|
|
da(ig)=fip*(tpiba2*ggp(ig)*ca(ig)+CMPLX(AIMAG(fp),-DBLE(fm)))
|
|
END DO
|
|
|
|
IF(dft_is_meta()) CALL dforce_meta(c,ca,df,da,psi,iss1,iss2,fi,fip) !METAGGA
|
|
!
|
|
! aa_i,i,n = sum_j d_i,ij <beta_i,j|c_n>
|
|
!
|
|
IF(nhsa.GT.0)THEN
|
|
DO inl=1,nhsa
|
|
af(inl)=0.
|
|
aa(inl)=0.
|
|
END DO
|
|
!
|
|
DO is=1,nsp
|
|
DO iv=1,nh(is)
|
|
DO jv=1,nh(is)
|
|
isa=0
|
|
DO ism=1,is-1
|
|
isa=isa+na(ism)
|
|
END DO
|
|
DO ia=1,na(is)
|
|
inl=ish(is)+(iv-1)*na(is)+ia
|
|
jnl=ish(is)+(jv-1)*na(is)+ia
|
|
isa=isa+1
|
|
dd = deeq(iv,jv,isa,iss1)+dvan(iv,jv,is)
|
|
IF(tens) THEN
|
|
af(inl)=af(inl)-dd*bec(jnl, i)
|
|
ELSE
|
|
af(inl)=af(inl)- f(i)*dd*bec(jnl, i)
|
|
END IF
|
|
dd = deeq(iv,jv,isa,iss2)+dvan(iv,jv,is)
|
|
IF(tens) THEN
|
|
IF (i.NE.n) aa(inl)=aa(inl)-dd*bec(jnl,i+1)
|
|
ELSE
|
|
IF (i.NE.n) aa(inl)=aa(inl)-f(i+1)*dd*bec(jnl,i+1)
|
|
END IF
|
|
END DO
|
|
END DO
|
|
END DO
|
|
END DO
|
|
!
|
|
DO ig=1,ngw
|
|
dtemp(ig)=(0.,0.)
|
|
END DO
|
|
CALL MXMA &
|
|
& (betae,1,2*ngw,af,1,nhsa,dtemp,1,2*ngw,2*ngw,nhsa,1)
|
|
DO ig=1,ngw
|
|
df(ig)=df(ig)+dtemp(ig)
|
|
END DO
|
|
!
|
|
DO ig=1,ngw
|
|
dtemp(ig)=(0.,0.)
|
|
END DO
|
|
CALL MXMA &
|
|
& (betae,1,2*ngw,aa,1,nhsa,dtemp,1,2*ngw,2*ngw,nhsa,1)
|
|
DO ig=1,ngw
|
|
da(ig)=da(ig)+dtemp(ig)
|
|
END DO
|
|
ENDIF
|
|
|
|
DEALLOCATE( psi )
|
|
!
|
|
CALL stop_clock( 'dforce' )
|
|
!
|
|
RETURN
|
|
END SUBROUTINE dforce
|
|
!
|
|
!-----------------------------------------------------------------------
|
|
SUBROUTINE dotcsc(eigr,cp)
|
|
!-----------------------------------------------------------------------
|
|
!
|
|
USE ions_base, ONLY: nas => nax, na, nsp, nat
|
|
USE io_global, ONLY: stdout
|
|
USE gvecw, ONLY: ngw
|
|
USE electrons_base, ONLY: n => nbsp
|
|
USE reciprocal_vectors, ONLY: gstart
|
|
USE cvan, ONLY: ish, nvb
|
|
USE uspp, ONLY: nhsa=>nkb, qq
|
|
USE uspp_param, ONLY: nh
|
|
USE mp, ONLY: mp_sum
|
|
USE mp_global, ONLY: intra_image_comm
|
|
!
|
|
IMPLICIT NONE
|
|
!
|
|
COMPLEX(8) eigr(ngw,nat), cp(ngw,n)
|
|
! local variables
|
|
REAL(8) rsum, csc(n) ! automatic array
|
|
COMPLEX(8) temp(ngw) ! automatic array
|
|
|
|
REAL(8), ALLOCATABLE:: becp(:,:)
|
|
INTEGER i,kmax,nnn,k,ig,is,ia,iv,jv,inl,jnl
|
|
!
|
|
ALLOCATE(becp(nhsa,n))
|
|
!
|
|
! < beta | phi > is real. only the i lowest:
|
|
!
|
|
nnn=MIN(12,n)
|
|
DO i=nnn,1,-1
|
|
kmax=i
|
|
CALL nlsm1(i,1,nvb,eigr,cp,becp)
|
|
!
|
|
DO k=1,kmax
|
|
DO ig=1,ngw
|
|
temp(ig)=CONJG(cp(ig,k))*cp(ig,i)
|
|
END DO
|
|
csc(k)=2.*DBLE(SUM(temp))
|
|
IF (gstart == 2) csc(k)=csc(k)-DBLE(temp(1))
|
|
END DO
|
|
|
|
CALL mp_sum( csc( 1:kmax ), intra_image_comm )
|
|
|
|
DO k=1,kmax
|
|
rsum=0.
|
|
DO is=1,nvb
|
|
DO iv=1,nh(is)
|
|
DO jv=1,nh(is)
|
|
DO ia=1,na(is)
|
|
inl=ish(is)+(iv-1)*na(is)+ia
|
|
jnl=ish(is)+(jv-1)*na(is)+ia
|
|
rsum = rsum + &
|
|
& qq(iv,jv,is)*becp(inl,i)*becp(jnl,k)
|
|
END DO
|
|
END DO
|
|
END DO
|
|
END DO
|
|
csc(k)=csc(k)+rsum
|
|
END DO
|
|
!
|
|
WRITE( stdout,'(a,12f18.15)')' dotcsc = ',(csc(k),k=1,i)
|
|
!
|
|
END DO
|
|
WRITE( stdout,*)
|
|
!
|
|
DEALLOCATE(becp)
|
|
!
|
|
RETURN
|
|
END SUBROUTINE dotcsc
|
|
!-----------------------------------------------------------------------
|
|
SUBROUTINE drhov(irb,eigrb,rhovan,rhog,rhor)
|
|
!-----------------------------------------------------------------------
|
|
! this routine calculates arrays drhog drhor, derivatives wrt h of:
|
|
!
|
|
! n_v(g) = sum_i,ij rho_i,ij q_i,ji(g) e^-ig.r_i
|
|
!
|
|
! Same logic as in routine rhov.
|
|
! On input rhor and rhog must contain the smooth part only !!!
|
|
! Output in module derho (drhor, drhog)
|
|
!
|
|
USE kinds, ONLY: dp
|
|
USE control_flags, ONLY: iprint
|
|
USE ions_base, ONLY: na, nsp, nat, nas => nax
|
|
USE cvan
|
|
USE uspp_param, ONLY: nhm, nh
|
|
USE grid_dimensions, ONLY: nr1, nr2, nr3, &
|
|
nr1x, nr2x, nr3x, nnr => nnrx
|
|
USE electrons_base, ONLY: nspin
|
|
USE gvecb
|
|
USE gvecp, ONLY: ng => ngm
|
|
USE smallbox_grid_dimensions, ONLY: nr1b, nr2b, nr3b, &
|
|
nr1bx, nr2bx, nr3bx, nnrb => nnrbx
|
|
USE cell_base, ONLY: ainv
|
|
USE qgb_mod
|
|
USE cdvan
|
|
USE derho
|
|
USE dqgb_mod
|
|
USE recvecs_indexes, ONLY: nm, np
|
|
USE fft_module, ONLY: fwfft, invfft
|
|
USE fft_base, ONLY: dfftb
|
|
|
|
IMPLICIT NONE
|
|
! input
|
|
INTEGER, INTENT(in) :: irb(3,nat)
|
|
REAL(8), INTENT(in):: rhor(nnr,nspin)
|
|
REAL(8) :: rhovan(nhm*(nhm+1)/2,nat,nspin)
|
|
COMPLEX(8), INTENT(in):: eigrb(ngb,nat), rhog(ng,nspin)
|
|
! local
|
|
INTEGER i, j, isup, isdw, nfft, ifft, iv, jv, ig, ijv, is, iss, &
|
|
& isa, ia, ir
|
|
REAL(8) sum, dsum
|
|
COMPLEX(8) fp, fm, ci
|
|
COMPLEX(8), ALLOCATABLE :: v(:)
|
|
COMPLEX(8), ALLOCATABLE:: dqgbt(:,:)
|
|
COMPLEX(8), ALLOCATABLE :: qv(:)
|
|
!
|
|
!
|
|
DO j=1,3
|
|
DO i=1,3
|
|
DO iss=1,nspin
|
|
DO ir=1,nnr
|
|
drhor(ir,iss,i,j)=-rhor(ir,iss)*ainv(j,i)
|
|
END DO
|
|
DO ig=1,ng
|
|
drhog(ig,iss,i,j)=-rhog(ig,iss)*ainv(j,i)
|
|
END DO
|
|
END DO
|
|
END DO
|
|
END DO
|
|
!
|
|
IF (nvb.EQ.0) RETURN
|
|
!
|
|
ALLOCATE( v( nnr ) )
|
|
ALLOCATE( qv( nnrb ) )
|
|
ALLOCATE( dqgbt( ngb, 2 ) )
|
|
|
|
ci=(0.,1.)
|
|
!
|
|
IF(nspin.EQ.1) THEN
|
|
! ------------------------------------------------------------------
|
|
! nspin=1 : two fft at a time, one per atom, if possible
|
|
! ------------------------------------------------------------------
|
|
DO i=1,3
|
|
DO j=1,3
|
|
!
|
|
v(:) = (0.d0, 0.d0)
|
|
!
|
|
iss=1
|
|
isa=1
|
|
DO is=1,nvb
|
|
#ifdef __PARA
|
|
DO ia=1,na(is)
|
|
nfft=1
|
|
IF ( dfftb%np3( isa ) <= 0 ) go to 15
|
|
#else
|
|
DO ia=1,na(is),2
|
|
nfft=2
|
|
#endif
|
|
dqgbt(:,:) = (0.d0, 0.d0)
|
|
IF (ia.EQ.na(is)) nfft=1
|
|
!
|
|
! nfft=2 if two ffts at the same time are performed
|
|
!
|
|
DO ifft=1,nfft
|
|
DO iv=1,nh(is)
|
|
DO jv=iv,nh(is)
|
|
ijv = (jv-1)*jv/2 + iv
|
|
sum = rhovan(ijv,isa+ifft-1,iss)
|
|
dsum=drhovan(ijv,isa+ifft-1,iss,i,j)
|
|
IF(iv.NE.jv) THEN
|
|
sum =2.*sum
|
|
dsum=2.*dsum
|
|
ENDIF
|
|
DO ig=1,ngb
|
|
dqgbt(ig,ifft)=dqgbt(ig,ifft) + &
|
|
& (sum*dqgb(ig,ijv,is,i,j) + &
|
|
& dsum*qgb(ig,ijv,is) )
|
|
END DO
|
|
END DO
|
|
END DO
|
|
END DO
|
|
!
|
|
! add structure factor
|
|
!
|
|
qv(:) = (0.d0, 0.d0)
|
|
IF(nfft.EQ.2) THEN
|
|
DO ig=1,ngb
|
|
qv(npb(ig)) = eigrb(ig,isa )*dqgbt(ig,1) &
|
|
& + ci* eigrb(ig,isa+1 )*dqgbt(ig,2)
|
|
qv(nmb(ig))= &
|
|
& CONJG(eigrb(ig,isa )*dqgbt(ig,1)) &
|
|
& + ci*CONJG(eigrb(ig,isa+1)*dqgbt(ig,2))
|
|
END DO
|
|
ELSE
|
|
DO ig=1,ngb
|
|
qv(npb(ig)) = eigrb(ig,isa)*dqgbt(ig,1)
|
|
qv(nmb(ig)) = &
|
|
& CONJG(eigrb(ig,isa)*dqgbt(ig,1))
|
|
END DO
|
|
ENDIF
|
|
!
|
|
CALL invfft('Box',qv,nr1b,nr2b,nr3b,nr1bx,nr2bx,nr3bx,isa)
|
|
!
|
|
! qv = US contribution in real space on box grid
|
|
! for atomic species is, real(qv)=atom ia, imag(qv)=atom ia+1
|
|
!
|
|
! add qv(r) to v(r), in real space on the dense grid
|
|
!
|
|
CALL box2grid(irb(1,isa),1,qv,v)
|
|
IF (nfft.EQ.2) CALL box2grid(irb(1,isa+1),2,qv,v)
|
|
15 isa=isa+nfft
|
|
!
|
|
END DO
|
|
END DO
|
|
!
|
|
DO ir=1,nnr
|
|
drhor(ir,iss,i,j)=drhor(ir,iss,i,j)+DBLE(v(ir))
|
|
END DO
|
|
!
|
|
CALL fwfft('Dense', v,nr1,nr2,nr3,nr1x,nr2x,nr3x)
|
|
!
|
|
DO ig=1,ng
|
|
drhog(ig,iss,i,j)=drhog(ig,iss,i,j)+v(np(ig))
|
|
END DO
|
|
!
|
|
ENDDO
|
|
ENDDO
|
|
!
|
|
ELSE
|
|
! ------------------------------------------------------------------
|
|
! nspin=2: two fft at a time, one for spin up and one for spin down
|
|
! ------------------------------------------------------------------
|
|
isup=1
|
|
isdw=2
|
|
DO i=1,3
|
|
DO j=1,3
|
|
v(:) = (0.d0, 0.d0)
|
|
isa=1
|
|
DO is=1,nvb
|
|
DO ia=1,na(is)
|
|
#ifdef __PARA
|
|
IF ( dfftb%np3( isa ) <= 0 ) go to 25
|
|
#endif
|
|
DO iss=1,2
|
|
dqgbt(:,iss) = (0.d0, 0.d0)
|
|
DO iv= 1,nh(is)
|
|
DO jv=iv,nh(is)
|
|
ijv = (jv-1)*jv/2 + iv
|
|
sum=rhovan(ijv,isa,iss)
|
|
dsum =drhovan(ijv,isa,iss,i,j)
|
|
IF(iv.NE.jv) THEN
|
|
sum =2.*sum
|
|
dsum=2.*dsum
|
|
ENDIF
|
|
DO ig=1,ngb
|
|
dqgbt(ig,iss)=dqgbt(ig,iss) + &
|
|
& (sum*dqgb(ig,ijv,is,i,j) + &
|
|
& dsum*qgb(ig,ijv,is))
|
|
END DO
|
|
END DO
|
|
END DO
|
|
END DO
|
|
!
|
|
! add structure factor
|
|
!
|
|
qv(:) = (0.d0, 0.d0)
|
|
DO ig=1,ngb
|
|
qv(npb(ig))= eigrb(ig,isa)*dqgbt(ig,1) &
|
|
& + ci* eigrb(ig,isa)*dqgbt(ig,2)
|
|
qv(nmb(ig))= CONJG(eigrb(ig,isa)*dqgbt(ig,1)) &
|
|
& + ci*CONJG(eigrb(ig,isa)*dqgbt(ig,2))
|
|
END DO
|
|
!
|
|
CALL invfft('Box',qv,nr1b,nr2b,nr3b,nr1bx,nr2bx,nr3bx,isa)
|
|
!
|
|
! qv is the now the US augmentation charge for atomic species is
|
|
! and atom ia: real(qv)=spin up, imag(qv)=spin down
|
|
!
|
|
! add qv(r) to v(r), in real space on the dense grid
|
|
!
|
|
CALL box2grid2(irb(1,isa),qv,v)
|
|
25 isa=isa+1
|
|
END DO
|
|
END DO
|
|
!
|
|
DO ir=1,nnr
|
|
drhor(ir,isup,i,j) = drhor(ir,isup,i,j) + DBLE(v(ir))
|
|
drhor(ir,isdw,i,j) = drhor(ir,isdw,i,j) +AIMAG(v(ir))
|
|
ENDDO
|
|
!
|
|
CALL fwfft('Dense', v,nr1,nr2,nr3,nr1x,nr2x,nr3x)
|
|
DO ig=1,ng
|
|
fp=v(np(ig))+v(nm(ig))
|
|
fm=v(np(ig))-v(nm(ig))
|
|
drhog(ig,isup,i,j) = drhog(ig,isup,i,j) + &
|
|
& 0.5*CMPLX( DBLE(fp),AIMAG(fm))
|
|
drhog(ig,isdw,i,j) = drhog(ig,isdw,i,j) + &
|
|
& 0.5*CMPLX(AIMAG(fp),-DBLE(fm))
|
|
END DO
|
|
!
|
|
END DO
|
|
END DO
|
|
ENDIF
|
|
DEALLOCATE(dqgbt)
|
|
DEALLOCATE( v )
|
|
DEALLOCATE( qv )
|
|
!
|
|
RETURN
|
|
END SUBROUTINE drhov
|
|
|
|
!
|
|
!-----------------------------------------------------------------------
|
|
FUNCTION enkin( c, ngwx, f, n )
|
|
!-----------------------------------------------------------------------
|
|
!
|
|
! calculation of kinetic energy term
|
|
!
|
|
USE kinds, ONLY: DP
|
|
USE constants, ONLY: pi, fpi
|
|
USE gvecw, ONLY: ngw
|
|
USE reciprocal_vectors, ONLY: gstart
|
|
USE gvecw, ONLY: ggp
|
|
USE mp, ONLY: mp_sum
|
|
USE mp_global, ONLY: intra_image_comm
|
|
USE cell_base, ONLY: tpiba2
|
|
|
|
IMPLICIT NONE
|
|
|
|
REAL(DP) :: enkin
|
|
|
|
! input
|
|
|
|
INTEGER, INTENT(IN) :: ngwx, n
|
|
COMPLEX(DP), INTENT(IN) :: c( ngwx, n )
|
|
REAL(DP), INTENT(IN) :: f( n )
|
|
!
|
|
! local
|
|
|
|
INTEGER :: ig, i
|
|
REAL(DP) :: sk(n) ! automatic array
|
|
!
|
|
DO i=1,n
|
|
sk(i)=0.0
|
|
DO ig=gstart,ngw
|
|
sk(i)=sk(i)+DBLE(CONJG(c(ig,i))*c(ig,i))*ggp(ig)
|
|
END DO
|
|
END DO
|
|
|
|
CALL mp_sum( sk(1:n), intra_image_comm )
|
|
|
|
enkin=0.0
|
|
DO i=1,n
|
|
enkin=enkin+f(i)*sk(i)
|
|
END DO
|
|
|
|
! ... reciprocal-space vectors are in units of alat/(2 pi) so a
|
|
! ... multiplicative factor (2 pi/alat)**2 is required
|
|
|
|
enkin = enkin * tpiba2
|
|
!
|
|
RETURN
|
|
END FUNCTION enkin
|
|
!
|
|
!
|
|
!-----------------------------------------------------------------------
|
|
SUBROUTINE force_ion(tau0,esr,fion,dsr)
|
|
!-----------------------------------------------------------------------
|
|
!
|
|
! forces on ions, ionic term in real space (also stress if requested)
|
|
!
|
|
USE control_flags, ONLY: iprint, tpre
|
|
USE constants, ONLY: pi, fpi
|
|
USE cell_base, ONLY: ainv, a1, a2, a3
|
|
USE ions_base, ONLY: nsp, na, rcmax, zv, nat
|
|
IMPLICIT NONE
|
|
! input
|
|
REAL(8) tau0(3,nat)
|
|
! output
|
|
REAL(8) fion(3,nat), dsr(3,3), esr
|
|
! local variables
|
|
INTEGER i,j,k,l,m, ii, lax, inf, isak, isaj
|
|
REAL(8) rlm(3), rckj, rlmn, arg, addesr, addpre, repand, fxx
|
|
REAL(8), EXTERNAL :: erfc
|
|
!
|
|
!
|
|
esr=0.d0
|
|
IF(tpre) dsr=0.d0
|
|
!
|
|
isak = 0
|
|
DO k=1,nsp
|
|
isaj = 0
|
|
DO j = 1, k-1
|
|
isaj = isaj + na(j)
|
|
END DO
|
|
DO j=k,nsp
|
|
rckj=SQRT(rcmax(k)**2+rcmax(j)**2)
|
|
lax=na(k)
|
|
IF(k.EQ.j) lax=lax-1
|
|
!
|
|
DO l=1,lax
|
|
inf=1
|
|
IF(k.EQ.j) inf=l+1
|
|
!
|
|
DO m=inf,na(j)
|
|
rlm(1) = tau0(1,l + isak) - tau0(1,m + isaj)
|
|
rlm(2) = tau0(2,l + isak) - tau0(2,m + isaj)
|
|
rlm(3) = tau0(3,l + isak) - tau0(3,m + isaj)
|
|
CALL pbc(rlm,a1,a2,a3,ainv,rlm)
|
|
!
|
|
rlmn=SQRT(rlm(1)**2+rlm(2)**2+rlm(3)**2)
|
|
!
|
|
arg=rlmn/rckj
|
|
addesr=zv(k)*zv(j)*erfc(arg)/rlmn
|
|
esr=esr+addesr
|
|
addpre=2.d0*zv(k)*zv(j)*EXP(-arg*arg)/rckj/SQRT(pi)
|
|
repand=(addesr+addpre)/rlmn/rlmn
|
|
!
|
|
DO i=1,3
|
|
fxx=repand*rlm(i)
|
|
fion(i,l+isak)=fion(i,l+isak)+fxx
|
|
fion(i,m+isaj)=fion(i,m+isaj)-fxx
|
|
IF(tpre)THEN
|
|
DO ii=1,3
|
|
dsr(i,ii)=dsr(i,ii)- &
|
|
& repand*rlm(i)*rlm(1)*ainv(ii,1)- &
|
|
& repand*rlm(i)*rlm(2)*ainv(ii,2)- &
|
|
& repand*rlm(i)*rlm(3)*ainv(ii,3)
|
|
END DO
|
|
ENDIF
|
|
END DO
|
|
END DO
|
|
END DO
|
|
isaj = isaj + na(j)
|
|
END DO
|
|
isak = isak + na(k)
|
|
END DO
|
|
|
|
RETURN
|
|
END SUBROUTINE force_ion
|
|
!
|
|
!-----------------------------------------------------------------------
|
|
SUBROUTINE force_ps(rhotemp,rhog,vtemp,ei1,ei2,ei3,fion1)
|
|
!-----------------------------------------------------------------------
|
|
!
|
|
! Contribution to ionic forces from local pseudopotential
|
|
!
|
|
USE kinds, ONLY: dp
|
|
USE constants, ONLY: pi, fpi
|
|
USE electrons_base, ONLY: nspin
|
|
USE gvecs
|
|
USE gvecp, ONLY: ng => ngm
|
|
USE reciprocal_vectors, ONLY: gstart, gx, mill_l, g
|
|
USE cell_base, ONLY: omega, tpiba, tpiba2
|
|
USE ions_base, ONLY: nsp, na, nas => nax, nat
|
|
USE grid_dimensions, ONLY: nr1, nr2, nr3
|
|
USE local_pseudo, ONLY: vps, rhops
|
|
!
|
|
IMPLICIT NONE
|
|
! input
|
|
COMPLEX(8) rhotemp(ng), rhog(ng,nspin), vtemp(ng), &
|
|
& ei1(-nr1:nr1,nat), &
|
|
& ei2(-nr2:nr2,nat), &
|
|
& ei3(-nr3:nr3,nat)
|
|
! output
|
|
REAL(8) fion1(3,nat)
|
|
! local
|
|
INTEGER ig, is, isa, ism, ia, ix, iss, isup, isdw
|
|
INTEGER i, j, k
|
|
REAL(8) wz
|
|
COMPLEX(8) eigrx, vcgs, cnvg, cvn
|
|
!
|
|
! wz = factor for g.neq.0 because of c*(g)=c(-g)
|
|
!
|
|
wz=2.0
|
|
DO is=1,nsp
|
|
isa=0
|
|
DO ism=1,is-1
|
|
isa=isa+na(ism)
|
|
END DO
|
|
DO ia=1,na(is)
|
|
isa=isa+1
|
|
DO ix=1,3
|
|
IF(nspin.EQ.1)THEN
|
|
iss=1
|
|
IF (gstart == 2) vtemp(1)=0.0
|
|
DO ig=gstart,ngs
|
|
vcgs=CONJG(rhotemp(ig))*fpi/(tpiba2*g(ig))
|
|
cnvg=rhops(ig,is)*vcgs
|
|
cvn=vps(ig,is)*CONJG(rhog(ig,iss))
|
|
i = mill_l(1,ig)
|
|
j = mill_l(2,ig)
|
|
k = mill_l(3,ig)
|
|
eigrx=ei1(i,isa)*ei2(j,isa)*ei3(k,isa)
|
|
vtemp(ig)=eigrx*(cnvg+cvn)*CMPLX(0.d0,gx(ix,ig))
|
|
END DO
|
|
ELSE
|
|
isup=1
|
|
isdw=2
|
|
IF (gstart == 2) vtemp(1)=0.0
|
|
DO ig=gstart,ngs
|
|
vcgs=CONJG(rhotemp(ig))*fpi/(tpiba2*g(ig))
|
|
cnvg=rhops(ig,is)*vcgs
|
|
cvn=vps(ig,is)*CONJG(rhog(ig,isup) &
|
|
& +rhog(ig,isdw))
|
|
i = mill_l(1,ig)
|
|
j = mill_l(2,ig)
|
|
k = mill_l(3,ig)
|
|
eigrx=ei1(i,isa)*ei2(j,isa)*ei3(k,isa)
|
|
vtemp(ig)=eigrx*(cnvg+cvn)*CMPLX(0.d0,gx(ix,ig))
|
|
END DO
|
|
ENDIF
|
|
fion1(ix,isa) = fion1(ix,isa) + tpiba*omega* wz*DBLE(SUM(vtemp))
|
|
END DO
|
|
END DO
|
|
END DO
|
|
!
|
|
RETURN
|
|
END SUBROUTINE force_ps
|
|
!
|
|
!-----------------------------------------------------------------------
|
|
SUBROUTINE gausin(eigr,cm)
|
|
!-----------------------------------------------------------------------
|
|
!
|
|
! initialize wavefunctions with gaussians - edit to fit your system
|
|
!
|
|
USE ions_base, ONLY: nas => nax, na, nsp, nat
|
|
USE electrons_base, ONLY: n => nbsp
|
|
USE gvecw, ONLY: ngw
|
|
USE reciprocal_vectors, ONLY: gx, g
|
|
!
|
|
IMPLICIT NONE
|
|
!
|
|
COMPLEX(8) eigr(ngw,nat), cm(ngw,n)
|
|
REAL(8) sigma, auxf
|
|
INTEGER nband, is, ia, ig, isa
|
|
!
|
|
sigma=12.0
|
|
nband=0
|
|
!!! do is=1,nsp
|
|
isa = 0
|
|
is=1
|
|
DO ia=1,na(is)
|
|
! s-like gaussians
|
|
nband=nband+1
|
|
DO ig=1,ngw
|
|
auxf=EXP(-g(ig)/sigma**2)
|
|
cm(ig,nband)=auxf*eigr(ig,ia+isa)
|
|
END DO
|
|
! px-like gaussians
|
|
nband=nband+1
|
|
DO ig=1,ngw
|
|
auxf=EXP(-g(ig)/sigma**2)
|
|
cm(ig,nband)=auxf*eigr(ig,ia+isa)*gx(1,ig)
|
|
END DO
|
|
! py-like gaussians
|
|
nband=nband+1
|
|
DO ig=1,ngw
|
|
auxf=EXP(-g(ig)/sigma**2)
|
|
cm(ig,nband)=auxf*eigr(ig,ia+isa)*gx(2,ig)
|
|
END DO
|
|
! pz-like gaussians
|
|
nband=nband+1
|
|
DO ig=1,ngw
|
|
auxf=EXP(-g(ig)/sigma**2)
|
|
cm(ig,nband)=auxf*eigr(ig,ia+isa)*gx(3,ig)
|
|
END DO
|
|
END DO
|
|
isa = isa + na(is)
|
|
is=2
|
|
DO ia=1,na(is)
|
|
! s-like gaussians
|
|
! nband=nband+1
|
|
! do ig=1,ngw
|
|
! auxf=exp(-g(ig)/sigma**2)
|
|
! cm(ig,nband)=auxf*eigr(ig,ia+isa)
|
|
! end do
|
|
! px-like gaussians
|
|
! nband=nband+1
|
|
! do ig=1,ngw
|
|
! auxf=exp(-g(ig)/sigma**2)
|
|
! cm(ig,nband)=auxf*eigr(ig,ia+isa)*gx(1,ig)
|
|
! end do
|
|
! py-like gaussians
|
|
! nband=nband+1
|
|
! do ig=1,ngw
|
|
! auxf=exp(-g(ig)/sigma**2)
|
|
! cm(ig,nband)=auxf*eigr(ig,ia+isa)*gx(2,ig)
|
|
! end do
|
|
! pz-like gaussians
|
|
! nband=nband+1
|
|
! do ig=1,ngw
|
|
! auxf=exp(-g(ig)/sigma**2)
|
|
! cm(ig,nband)=auxf*eigr(ig,ia+isa)*gx(3,ig)
|
|
! end do
|
|
! dxy-like gaussians
|
|
! nband=nband+1
|
|
! do ig=1,ngw
|
|
! auxf=exp(-g(ig)/sigma**2)
|
|
! cm(ig,nband)=auxf*eigr(ig,ia+isa)*gx(1,ig)*gx(2,ig)
|
|
! end do
|
|
! dxz-like gaussians
|
|
! nband=nband+1
|
|
! do ig=1,ngw
|
|
! auxf=exp(-g(ig)/sigma**2)
|
|
! cm(ig,nband)=auxf*eigr(ig,ia+isa)*gx(1,ig)*gx(3,ig)
|
|
! end do
|
|
! dxy-like gaussians
|
|
! nband=nband+1
|
|
! do ig=1,ngw
|
|
! auxf=exp(-g(ig)/sigma**2)
|
|
! cm(ig,nband)=auxf*eigr(ig,ia+isa)*gx(2,ig)*gx(3,ig)
|
|
! end do
|
|
! dx2-y2-like gaussians
|
|
! nband=nband+1
|
|
! do ig=1,ngw
|
|
! auxf=exp(-g(ig)/sigma**2)
|
|
! cm(ig,nband)=auxf*eigr(ig,ia+isa)* &
|
|
! & (gx(1,ig)**2-gx(2,ig)**2)
|
|
! end do
|
|
END DO
|
|
!!! end do
|
|
RETURN
|
|
END SUBROUTINE gausin
|
|
!
|
|
|
|
!-------------------------------------------------------------------------
|
|
SUBROUTINE gracsc( bec, nkbx, betae, cp, ngwx, i, csc, n )
|
|
!-----------------------------------------------------------------------
|
|
! requires in input the updated bec(k) for k<i
|
|
! on output: bec(i) is recalculated
|
|
!
|
|
USE ions_base, ONLY: na
|
|
USE cvan, ONLY :nvb, ish
|
|
USE uspp, ONLY : nkb, nhsavb=>nkbus, qq
|
|
USE uspp_param, ONLY: nh
|
|
USE electrons_base, ONLY: ispin
|
|
USE gvecw, ONLY: ngw
|
|
USE mp, ONLY: mp_sum
|
|
USE mp_global, ONLY: intra_image_comm
|
|
USE kinds, ONLY: DP
|
|
USE reciprocal_vectors, ONLY: gstart
|
|
!
|
|
IMPLICIT NONE
|
|
!
|
|
INTEGER, INTENT(IN) :: i, nkbx, ngwx, n
|
|
COMPLEX(DP) :: betae( ngwx, nkb )
|
|
REAL(DP) :: bec( nkbx, n ), cp( 2, ngwx, n )
|
|
REAL(DP) :: csc( n )
|
|
INTEGER :: k, kmax,ig, is, iv, jv, ia, inl, jnl
|
|
REAL(DP) :: rsum
|
|
REAL(DP), ALLOCATABLE :: temp(:)
|
|
|
|
!
|
|
! calculate csc(k)=<cp(i)|cp(k)>, k<i
|
|
!
|
|
ALLOCATE( temp( ngw ) )
|
|
|
|
kmax = i - 1
|
|
|
|
DO k = 1, kmax
|
|
csc(k) = 0.0d0
|
|
IF ( ispin(i) .EQ. ispin(k) ) THEN
|
|
DO ig = 1, ngw
|
|
temp(ig) = cp(1,ig,k) * cp(1,ig,i) + cp(2,ig,k) * cp(2,ig,i)
|
|
END DO
|
|
csc(k) = 2.0d0 * SUM(temp)
|
|
IF (gstart == 2) csc(k) = csc(k) - temp(1)
|
|
ENDIF
|
|
END DO
|
|
|
|
CALL mp_sum( csc( 1:kmax ), intra_image_comm )
|
|
|
|
!
|
|
! calculate bec(i)=<cp(i)|beta>
|
|
!
|
|
DO inl=1,nhsavb
|
|
DO ig=1,ngw
|
|
temp(ig)=cp(1,ig,i)* DBLE(betae(ig,inl))+ &
|
|
& cp(2,ig,i)*AIMAG(betae(ig,inl))
|
|
END DO
|
|
bec(inl,i)=2.*SUM(temp)
|
|
IF (gstart == 2) bec(inl,i)= bec(inl,i)-temp(1)
|
|
END DO
|
|
|
|
CALL mp_sum( bec( 1:nhsavb, i ), intra_image_comm )
|
|
!
|
|
! calculate csc(k)=<cp(i)|S|cp(k)>, k<i
|
|
!
|
|
DO k=1,kmax
|
|
IF (ispin(i).EQ.ispin(k)) THEN
|
|
rsum=0.
|
|
DO is=1,nvb
|
|
DO iv=1,nh(is)
|
|
DO jv=1,nh(is)
|
|
IF(ABS(qq(iv,jv,is)).GT.1.e-5) THEN
|
|
DO ia=1,na(is)
|
|
inl=ish(is)+(iv-1)*na(is)+ia
|
|
jnl=ish(is)+(jv-1)*na(is)+ia
|
|
rsum = rsum + qq(iv,jv,is)*bec(inl,i)*bec(jnl,k)
|
|
END DO
|
|
ENDIF
|
|
END DO
|
|
END DO
|
|
END DO
|
|
csc(k)=csc(k)+rsum
|
|
ENDIF
|
|
END DO
|
|
!
|
|
! orthogonalized cp(i) : |cp(i)>=|cp(i)>-\sum_k<i csc(k)|cp(k)>
|
|
!
|
|
! corresponing bec: bec(i)=<cp(i)|beta>-csc(k)<cp(k)|beta>
|
|
!
|
|
DO k=1,kmax
|
|
DO inl=1,nkbx
|
|
bec(inl,i)=bec(inl,i)-csc(k)*bec(inl,k)
|
|
END DO
|
|
END DO
|
|
|
|
DEALLOCATE( temp )
|
|
!
|
|
RETURN
|
|
END SUBROUTINE gracsc
|
|
|
|
!-------------------------------------------------------------------------
|
|
SUBROUTINE gram( betae, bec, nkbx, cp, ngwx, n )
|
|
!-----------------------------------------------------------------------
|
|
! gram-schmidt orthogonalization of the set of wavefunctions cp
|
|
!
|
|
USE uspp, ONLY : nkb, nhsavb=> nkbus
|
|
USE gvecw, ONLY : ngw
|
|
USE kinds, ONLY : DP
|
|
!
|
|
IMPLICIT NONE
|
|
!
|
|
INTEGER, INTENT(IN) :: nkbx, ngwx, n
|
|
REAL(DP) :: bec( nkbx, n )
|
|
COMPLEX(DP) :: cp( ngwx, n ), betae( ngwx, nkb )
|
|
!
|
|
REAL(DP) :: anorm, cscnorm
|
|
REAL(DP), ALLOCATABLE :: csc( : )
|
|
INTEGER :: i,k
|
|
EXTERNAL cscnorm
|
|
!
|
|
CALL start_clock( 'gram' )
|
|
|
|
ALLOCATE( csc( n ) )
|
|
!
|
|
DO i = 1, n
|
|
!
|
|
CALL gracsc( bec, nkbx, betae, cp, ngwx, i, csc, n )
|
|
!
|
|
! calculate orthogonalized cp(i) : |cp(i)>=|cp(i)>-\sum_k<i csc(k)|cp(k)>
|
|
!
|
|
DO k = 1, i - 1
|
|
CALL DAXPY( 2*ngw, -csc(k), cp(1,k), 1, cp(1,i), 1 )
|
|
END DO
|
|
anorm = cscnorm( bec, nkbx, cp, ngwx, i, n )
|
|
CALL DSCAL( 2*ngw, 1.0/anorm, cp(1,i), 1 )
|
|
!
|
|
! these are the final bec's
|
|
!
|
|
CALL DSCAL( nkbx, 1.0/anorm, bec(1,i), 1 )
|
|
END DO
|
|
!
|
|
DEALLOCATE( csc )
|
|
|
|
CALL stop_clock( 'gram' )
|
|
!
|
|
RETURN
|
|
END SUBROUTINE gram
|
|
!
|
|
!-----------------------------------------------------------------------
|
|
SUBROUTINE initbox ( tau0, taub, irb )
|
|
!-----------------------------------------------------------------------
|
|
!
|
|
! sets the indexes irb and positions taub for the small boxes
|
|
! around atoms
|
|
!
|
|
USE ions_base, ONLY: nsp, na, nat
|
|
USE grid_dimensions, ONLY: nr1, nr2, nr3
|
|
USE cell_base, ONLY: ainv, a1, a2, a3
|
|
USE smallbox_grid_dimensions, ONLY: nr1b, nr2b, nr3b, nr1bx, nr2bx, nr3bx
|
|
USE control_flags, ONLY: iprsta
|
|
USE io_global, ONLY: stdout
|
|
USE mp_global, ONLY: nproc_image, me_image
|
|
USE fft_base, ONLY: dfftb, dfftp, fft_dlay_descriptor
|
|
USE fft_types, ONLY: fft_box_set
|
|
USE cvan, ONLY: nvb
|
|
|
|
IMPLICIT NONE
|
|
! input
|
|
REAL(8), INTENT(in):: tau0(3,nat)
|
|
! output
|
|
INTEGER, INTENT(out):: irb(3,nat)
|
|
REAL(8), INTENT(out):: taub(3,nat)
|
|
! local
|
|
REAL(8) x(3), xmod
|
|
INTEGER nr(3), nrb(3), xint, is, ia, i, isa
|
|
!
|
|
nr (1)=nr1
|
|
nr (2)=nr2
|
|
nr (3)=nr3
|
|
nrb(1)=nr1b
|
|
nrb(2)=nr2b
|
|
nrb(3)=nr3b
|
|
!
|
|
isa = 0
|
|
DO is=1,nsp
|
|
DO ia=1,na(is)
|
|
isa = isa + 1
|
|
!
|
|
DO i=1,3
|
|
!
|
|
! bring atomic positions to crystal axis
|
|
!
|
|
x(i) = ainv(i,1)*tau0(1,isa) + &
|
|
& ainv(i,2)*tau0(2,isa) + &
|
|
& ainv(i,3)*tau0(3,isa)
|
|
!
|
|
! bring x in the range between 0 and 1
|
|
!
|
|
x(i) = MOD(x(i),1.d0)
|
|
IF (x(i).LT.0.d0) x(i)=x(i)+1.d0
|
|
!
|
|
! case of nrb(i) even
|
|
!
|
|
IF (MOD(nrb(i),2).EQ.0) THEN
|
|
!
|
|
! find irb = index of the grid point at the corner of the small box
|
|
! (the indices of the small box run from irb to irb+nrb-1)
|
|
!
|
|
xint=INT(x(i)*nr(i))
|
|
irb (i,isa)=xint+1-nrb(i)/2+1
|
|
IF(irb(i,isa).LT.1) irb(i,isa)=irb(i,isa)+nr(i)
|
|
!
|
|
! x(i) are the atomic positions in crystal coordinates, where the
|
|
! "crystal lattice" is the small box lattice and the origin is at
|
|
! the corner of the small box. Used to calculate phases exp(iG*taub)
|
|
!
|
|
xmod=x(i)*nr(i)-xint
|
|
x(i)=(xmod+nrb(i)/2-1)/nr(i)
|
|
ELSE
|
|
!
|
|
! case of nrb(i) odd - see above for comments
|
|
!
|
|
xint=NINT(x(i)*nr(i))
|
|
irb (i,isa)=xint+1-(nrb(i)-1)/2
|
|
IF(irb(i,isa).LT.1) irb(i,isa)=irb(i,isa)+nr(i)
|
|
xmod=x(i)*nr(i)-xint
|
|
x(i)=(xmod+(nrb(i)-1)/2)/nr(i)
|
|
END IF
|
|
END DO
|
|
!
|
|
! bring back taub in cartesian coordinates
|
|
!
|
|
DO i=1,3
|
|
taub(i,isa)= x(1)*a1(i) + x(2)*a2(i) + x(3)*a3(i)
|
|
END DO
|
|
END DO
|
|
END DO
|
|
|
|
CALL fft_box_set( dfftb, nr1b, nr2b, nr3b, nr1bx, nr2bx, nr3bx, &
|
|
nat, irb, me_image+1, nproc_image, dfftp%npp, dfftp%ipp )
|
|
|
|
IF( iprsta > 2 ) THEN
|
|
isa = 1
|
|
DO is=1,nsp
|
|
WRITE( stdout,'(/,2x,''species= '',i2)') is
|
|
DO ia=1,na(is)
|
|
WRITE( stdout,2000) ia, (irb(i,isa),i=1,3)
|
|
2000 FORMAT(2x,'atom= ',i3,' irb1= ',i3,' irb2= ',i3,' irb3= ',i3)
|
|
isa = isa + 1
|
|
END DO
|
|
END DO
|
|
ENDIF
|
|
|
|
#ifdef __PARA
|
|
!
|
|
! for processor that do not call fft on the box
|
|
! artificially start the clock
|
|
!
|
|
isa=1
|
|
DO is=1,nvb
|
|
DO ia=1,na(is)
|
|
IF ( dfftb%np3( isa ) <= 0 ) then
|
|
CALL start_clock( 'fftb' )
|
|
CALL stop_clock( 'fftb' )
|
|
END IF
|
|
isa = isa + 1
|
|
END DO
|
|
END DO
|
|
#endif
|
|
!
|
|
RETURN
|
|
END SUBROUTINE initbox
|
|
!
|
|
!-------------------------------------------------------------------------
|
|
SUBROUTINE newd(vr,irb,eigrb,rhovan,fion)
|
|
!-----------------------------------------------------------------------
|
|
! this routine calculates array deeq:
|
|
! deeq_i,lm = \int V_eff(r) q_i,lm(r) dr
|
|
! and the corresponding term in forces
|
|
! fion_i = \int V_eff(r) \sum_lm rho_lm (dq_i,lm(r)/dR_i) dr
|
|
! where
|
|
! rho_lm = \sum_j f_j <psi_j|beta_l><beta_m|psi_j>
|
|
!
|
|
USE kinds, ONLY: dp
|
|
USE uspp_param, ONLY: nh, nhm
|
|
USE uspp, ONLY: deeq
|
|
USE cvan, ONLY: nvb
|
|
USE ions_base, ONLY: nas => nax, nat, nsp, na
|
|
USE parameters, ONLY: nsx
|
|
USE constants, ONLY: pi, fpi
|
|
USE grid_dimensions, ONLY: nr3, nnr => nnrx
|
|
USE gvecb
|
|
USE small_box, ONLY: omegab, tpibab
|
|
USE smallbox_grid_dimensions, ONLY: nr1b, nr2b, nr3b, &
|
|
nr1bx, nr2bx, nr3bx, nnrb => nnrbx
|
|
USE qgb_mod
|
|
USE electrons_base, ONLY: nspin
|
|
USE control_flags, ONLY: iprint, thdyn, tfor, tprnfor
|
|
USE mp, ONLY: mp_sum
|
|
USE mp_global, ONLY: intra_image_comm
|
|
USE fft_module, ONLY: invfft
|
|
USE fft_base, ONLY: dfftb
|
|
!
|
|
IMPLICIT NONE
|
|
! input
|
|
INTEGER irb(3,nat)
|
|
REAL(8) rhovan(nhm*(nhm+1)/2,nat,nspin)
|
|
COMPLEX(8) eigrb(ngb,nat)
|
|
REAL(8) vr(nnr,nspin)
|
|
! output
|
|
REAL(8) fion(3,nat)
|
|
! local
|
|
INTEGER isup,isdw,iss, iv,ijv,jv, ik, nfft, isa, ia, is, ig
|
|
REAL(8) fvan(3,nat,nsx), fac, fac1, fac2, boxdotgrid
|
|
COMPLEX(8) ci, facg1, facg2
|
|
COMPLEX(8), ALLOCATABLE :: qv(:)
|
|
EXTERNAL boxdotgrid
|
|
!
|
|
CALL start_clock( 'newd' )
|
|
ci=(0.d0,1.d0)
|
|
fac=omegab/DBLE(nr1b*nr2b*nr3b)
|
|
deeq (:,:,:,:) = 0.d0
|
|
fvan (:,:,:) = 0.d0
|
|
|
|
ALLOCATE( qv( nnrb ) )
|
|
!
|
|
! calculation of deeq_i,lm = \int V_eff(r) q_i,lm(r) dr
|
|
!
|
|
isa=1
|
|
DO is=1,nvb
|
|
#ifdef __PARA
|
|
DO ia=1,na(is)
|
|
nfft=1
|
|
IF ( dfftb%np3( isa ) <= 0 ) go to 15
|
|
#else
|
|
DO ia=1,na(is),2
|
|
nfft=2
|
|
#endif
|
|
IF( ia .EQ. na(is) ) nfft=1
|
|
!
|
|
! two ffts at the same time, on two atoms (if possible: nfft=2)
|
|
!
|
|
DO iv=1,nh(is)
|
|
DO jv=iv,nh(is)
|
|
ijv = (jv-1)*jv/2 + iv
|
|
qv(:) = (0.d0, 0.d0)
|
|
IF (nfft.EQ.2) THEN
|
|
DO ig=1,ngb
|
|
qv(npb(ig))= eigrb(ig,isa )*qgb(ig,ijv,is) &
|
|
& + ci*eigrb(ig,isa+1)*qgb(ig,ijv,is)
|
|
qv(nmb(ig))= CONJG( &
|
|
& eigrb(ig,isa )*qgb(ig,ijv,is)) &
|
|
& + ci*CONJG( &
|
|
& eigrb(ig,isa+1)*qgb(ig,ijv,is))
|
|
END DO
|
|
ELSE
|
|
DO ig=1,ngb
|
|
qv(npb(ig)) = eigrb(ig,isa)*qgb(ig,ijv,is)
|
|
qv(nmb(ig)) = CONJG( &
|
|
& eigrb(ig,isa)*qgb(ig,ijv,is))
|
|
END DO
|
|
END IF
|
|
!
|
|
CALL invfft('Box',qv,nr1b,nr2b,nr3b,nr1bx,nr2bx,nr3bx,isa)
|
|
!
|
|
DO iss=1,nspin
|
|
deeq(iv,jv,isa,iss) = fac * &
|
|
& boxdotgrid(irb(1,isa),1,qv,vr(1,iss))
|
|
IF (iv.NE.jv) &
|
|
& deeq(jv,iv,isa,iss)=deeq(iv,jv,isa,iss)
|
|
!
|
|
IF (nfft.EQ.2) THEN
|
|
deeq(iv,jv,isa+1,iss) = fac* &
|
|
& boxdotgrid(irb(1,isa+1),2,qv,vr(1,iss))
|
|
IF (iv.NE.jv) &
|
|
& deeq(jv,iv,isa+1,iss)=deeq(iv,jv,isa+1,iss)
|
|
END IF
|
|
END DO
|
|
END DO
|
|
END DO
|
|
15 isa=isa+nfft
|
|
END DO
|
|
END DO
|
|
|
|
CALL mp_sum( deeq, intra_image_comm )
|
|
|
|
IF (.NOT.( tfor .OR. thdyn .OR. tprnfor ) ) go to 10
|
|
!
|
|
! calculation of fion_i = \int V_eff(r) \sum_lm rho_lm (dq_i,lm(r)/dR_i) dr
|
|
!
|
|
isa=1
|
|
IF(nspin.EQ.1) THEN
|
|
! =================================================================
|
|
! case nspin=1: two ffts at the same time, on two atoms (if possible)
|
|
! -----------------------------------------------------------------
|
|
iss=1
|
|
isa=1
|
|
DO is=1,nvb
|
|
#ifdef __PARA
|
|
DO ia=1,na(is)
|
|
nfft=1
|
|
IF ( dfftb%np3( isa ) <= 0 ) go to 20
|
|
#else
|
|
DO ia=1,na(is),2
|
|
nfft=2
|
|
#endif
|
|
IF( ia.EQ.na(is)) nfft=1
|
|
DO ik=1,3
|
|
qv(:) = (0.d0, 0.d0)
|
|
DO iv=1,nh(is)
|
|
DO jv=iv,nh(is)
|
|
ijv = (jv-1)*jv/2 + iv
|
|
IF(iv.NE.jv) THEN
|
|
fac1=2.d0*fac*tpibab*rhovan(ijv,isa,iss)
|
|
IF (nfft.EQ.2) fac2=2.d0*fac*tpibab* &
|
|
& rhovan(ijv,isa+1,iss)
|
|
ELSE
|
|
fac1= fac*tpibab*rhovan(ijv,isa,iss)
|
|
IF (nfft.EQ.2) fac2= fac*tpibab* &
|
|
& rhovan(ijv,isa+1,iss)
|
|
ENDIF
|
|
IF (nfft.EQ.2) THEN
|
|
DO ig=1,ngb
|
|
facg1 = CMPLX(0.d0,-gxb(ik,ig)) * &
|
|
& qgb(ig,ijv,is) * fac1
|
|
facg2 = CMPLX(0.d0,-gxb(ik,ig)) * &
|
|
& qgb(ig,ijv,is) * fac2
|
|
qv(npb(ig)) = qv(npb(ig)) &
|
|
& + eigrb(ig,isa )*facg1 &
|
|
& + ci*eigrb(ig,isa+1)*facg2
|
|
qv(nmb(ig)) = qv(nmb(ig)) &
|
|
& + CONJG(eigrb(ig,isa )*facg1)&
|
|
& +ci*CONJG(eigrb(ig,isa+1)*facg2)
|
|
END DO
|
|
ELSE
|
|
DO ig=1,ngb
|
|
facg1 = CMPLX(0.d0,-gxb(ik,ig)) * &
|
|
& qgb(ig,ijv,is)*fac1
|
|
qv(npb(ig)) = qv(npb(ig)) &
|
|
& + eigrb(ig,isa)*facg1
|
|
qv(nmb(ig)) = qv(nmb(ig)) &
|
|
& + CONJG( eigrb(ig,isa)*facg1)
|
|
END DO
|
|
END IF
|
|
END DO
|
|
END DO
|
|
!
|
|
CALL invfft('Box',qv,nr1b,nr2b,nr3b,nr1bx,nr2bx,nr3bx,isa)
|
|
!
|
|
fvan(ik,ia,is) = &
|
|
& boxdotgrid(irb(1,isa),1,qv,vr(1,iss))
|
|
!
|
|
IF (nfft.EQ.2) fvan(ik,ia+1,is) = &
|
|
& boxdotgrid(irb(1,isa+1),2,qv,vr(1,iss))
|
|
END DO
|
|
20 isa = isa+nfft
|
|
END DO
|
|
END DO
|
|
ELSE
|
|
! =================================================================
|
|
! case nspin=2: up and down spin fft's combined into a single fft
|
|
! -----------------------------------------------------------------
|
|
isup=1
|
|
isdw=2
|
|
isa=1
|
|
DO is=1,nvb
|
|
DO ia=1,na(is)
|
|
#ifdef __PARA
|
|
IF ( dfftb%np3( isa ) <= 0 ) go to 25
|
|
#endif
|
|
DO ik=1,3
|
|
qv(:) = (0.d0, 0.d0)
|
|
!
|
|
DO iv=1,nh(is)
|
|
DO jv=iv,nh(is)
|
|
ijv = (jv-1)*jv/2 + iv
|
|
IF(iv.NE.jv) THEN
|
|
fac1=2.d0*fac*tpibab*rhovan(ijv,isa,isup)
|
|
fac2=2.d0*fac*tpibab*rhovan(ijv,isa,isdw)
|
|
ELSE
|
|
fac1= fac*tpibab*rhovan(ijv,isa,isup)
|
|
fac2= fac*tpibab*rhovan(ijv,isa,isdw)
|
|
END IF
|
|
DO ig=1,ngb
|
|
facg1 = fac1 * CMPLX(0.d0,-gxb(ik,ig)) * &
|
|
& qgb(ig,ijv,is) * eigrb(ig,isa)
|
|
facg2 = fac2 * CMPLX(0.d0,-gxb(ik,ig)) * &
|
|
& qgb(ig,ijv,is) * eigrb(ig,isa)
|
|
qv(npb(ig)) = qv(npb(ig)) &
|
|
& + facg1 + ci*facg2
|
|
qv(nmb(ig)) = qv(nmb(ig)) &
|
|
& +CONJG(facg1)+ci*CONJG(facg2)
|
|
END DO
|
|
END DO
|
|
END DO
|
|
!
|
|
CALL invfft('Box',qv,nr1b,nr2b,nr3b,nr1bx,nr2bx,nr3bx,isa)
|
|
!
|
|
fvan(ik,ia,is) = &
|
|
& boxdotgrid(irb(1,isa),isup,qv,vr(1,isup)) + &
|
|
& boxdotgrid(irb(1,isa),isdw,qv,vr(1,isdw))
|
|
END DO
|
|
25 isa = isa+1
|
|
END DO
|
|
END DO
|
|
END IF
|
|
|
|
CALL mp_sum( fvan, intra_image_comm )
|
|
|
|
isa = 0
|
|
DO is = 1, nvb
|
|
DO ia = 1, na(is)
|
|
isa = isa + 1
|
|
fion(:,isa) = fion(:,isa) - fvan(:,ia,is)
|
|
END DO
|
|
END DO
|
|
|
|
DEALLOCATE( qv )
|
|
!
|
|
10 CALL stop_clock( 'newd' )
|
|
!
|
|
RETURN
|
|
END SUBROUTINE newd
|
|
!-------------------------------------------------------------------------
|
|
SUBROUTINE nlfl(bec,becdr,lambda,fion)
|
|
!-----------------------------------------------------------------------
|
|
! contribution to fion due to the orthonormality constraint
|
|
!
|
|
!
|
|
USE io_global, ONLY: stdout
|
|
USE ions_base, ONLY: na, nsp, nat
|
|
USE uspp, ONLY :nhsa=>nkb, qq
|
|
USE uspp_param, ONLY: nhm, nh
|
|
USE cvan, ONLY: ish, nvb
|
|
USE electrons_base, ONLY: nbspx, nbsp, nudx, nspin, iupdwn, nupdwn
|
|
USE constants, ONLY: pi, fpi
|
|
!
|
|
IMPLICIT NONE
|
|
REAL(8) bec(nhsa,nbsp), becdr(nhsa,nbsp,3), lambda(nudx,nudx,nspin)
|
|
REAL(8) fion(3,nat)
|
|
!
|
|
INTEGER k, is, ia, iv, jv, i, j, inl, isa, iss, nss, istart
|
|
REAL(8), ALLOCATABLE :: temp(:,:), tmpbec(:,:),tmpdr(:,:)
|
|
!
|
|
CALL start_clock( 'nlfl' )
|
|
!
|
|
ALLOCATE( temp( nudx, nudx ), tmpbec( nhm, nudx ), tmpdr( nudx, nhm ) )
|
|
|
|
DO k=1,3
|
|
isa = 0
|
|
DO is=1,nvb
|
|
DO ia=1,na(is)
|
|
isa = isa + 1
|
|
!
|
|
DO iss = 1, nspin
|
|
!
|
|
nss = nupdwn( iss )
|
|
istart = iupdwn( iss )
|
|
!
|
|
tmpbec = 0.d0
|
|
tmpdr = 0.d0
|
|
!
|
|
DO iv=1,nh(is)
|
|
DO jv=1,nh(is)
|
|
inl=ish(is)+(jv-1)*na(is)+ia
|
|
IF(ABS(qq(iv,jv,is)).GT.1.e-5) THEN
|
|
DO i=1,nss
|
|
tmpbec(iv,i)=tmpbec(iv,i) &
|
|
& + qq(iv,jv,is)*bec(inl,i+istart-1)
|
|
END DO
|
|
ENDIF
|
|
END DO
|
|
END DO
|
|
!
|
|
DO iv=1,nh(is)
|
|
inl=ish(is)+(iv-1)*na(is)+ia
|
|
DO i=1,nss
|
|
tmpdr(i,iv)=becdr(inl,i+istart-1,k)
|
|
END DO
|
|
END DO
|
|
!
|
|
IF(nh(is).GT.0)THEN
|
|
!
|
|
temp = 0.d0
|
|
!
|
|
CALL MXMA &
|
|
& (tmpdr,1,nudx,tmpbec,1,nhm,temp,1,nudx,nss,nh(is),nss)
|
|
!
|
|
DO j=1,nss
|
|
DO i=1,nss
|
|
temp(i,j)=temp(i,j)*lambda(i,j,iss)
|
|
END DO
|
|
END DO
|
|
!
|
|
fion(k,isa)=fion(k,isa)+2.*SUM(temp)
|
|
ENDIF
|
|
|
|
END DO
|
|
!
|
|
END DO
|
|
END DO
|
|
END DO
|
|
!
|
|
! end of x/y/z loop
|
|
|
|
DEALLOCATE( temp, tmpbec, tmpdr )
|
|
!
|
|
CALL stop_clock( 'nlfl' )
|
|
!
|
|
RETURN
|
|
END SUBROUTINE nlfl
|
|
|
|
!
|
|
!-----------------------------------------------------------------------
|
|
SUBROUTINE pbc(rin,a1,a2,a3,ainv,rout)
|
|
!-----------------------------------------------------------------------
|
|
!
|
|
! brings atoms inside the unit cell
|
|
!
|
|
IMPLICIT NONE
|
|
! input
|
|
REAL(8) rin(3), a1(3),a2(3),a3(3), ainv(3,3)
|
|
! output
|
|
REAL(8) rout(3)
|
|
! local
|
|
REAL(8) x,y,z
|
|
!
|
|
! bring atomic positions to crystal axis
|
|
!
|
|
x = ainv(1,1)*rin(1)+ainv(1,2)*rin(2)+ainv(1,3)*rin(3)
|
|
y = ainv(2,1)*rin(1)+ainv(2,2)*rin(2)+ainv(2,3)*rin(3)
|
|
z = ainv(3,1)*rin(1)+ainv(3,2)*rin(2)+ainv(3,3)*rin(3)
|
|
!
|
|
! bring x,y,z in the range between -0.5 and 0.5
|
|
!
|
|
x = x - NINT(x)
|
|
y = y - NINT(y)
|
|
z = z - NINT(z)
|
|
!
|
|
! bring atomic positions back in cartesian axis
|
|
!
|
|
rout(1) = x*a1(1)+y*a2(1)+z*a3(1)
|
|
rout(2) = x*a1(2)+y*a2(2)+z*a3(2)
|
|
rout(3) = x*a1(3)+y*a2(3)+z*a3(3)
|
|
!
|
|
RETURN
|
|
END SUBROUTINE pbc
|
|
|
|
!
|
|
!-------------------------------------------------------------------------
|
|
SUBROUTINE prefor(eigr,betae)
|
|
!-----------------------------------------------------------------------
|
|
!
|
|
! input : eigr = e^-ig.r_i
|
|
! output: betae_i,i(g) = (-i)**l beta_i,i(g) e^-ig.r_i
|
|
!
|
|
USE ions_base, ONLY: nas => nax, nsp, na, nat
|
|
USE gvecw, ONLY: ngw
|
|
USE cvan, ONLY: ish
|
|
USE uspp, ONLY :nhsa=>nkb, beta, nhtol
|
|
USE uspp_param, ONLY: nh
|
|
!
|
|
IMPLICIT NONE
|
|
COMPLEX(8) eigr(ngw,nat)
|
|
COMPLEX(8) betae(ngw,nhsa)
|
|
!
|
|
INTEGER is, iv, ia, inl, ig, isa
|
|
COMPLEX(8) ci
|
|
!
|
|
CALL start_clock( 'prefor' )
|
|
isa = 0
|
|
DO is=1,nsp
|
|
DO iv=1,nh(is)
|
|
ci=(0.,-1.)**nhtol(iv,is)
|
|
DO ia=1,na(is)
|
|
inl=ish(is)+(iv-1)*na(is)+ia
|
|
DO ig=1,ngw
|
|
betae(ig,inl)=ci*beta(ig,iv,is)*eigr(ig,ia+isa)
|
|
END DO
|
|
END DO
|
|
END DO
|
|
isa = isa + na(is)
|
|
END DO
|
|
CALL stop_clock( 'prefor' )
|
|
!
|
|
RETURN
|
|
END SUBROUTINE prefor
|
|
!
|
|
!-----------------------------------------------------------------------
|
|
SUBROUTINE projwfc(c,eigr,betae)
|
|
!-----------------------------------------------------------------------
|
|
!
|
|
! Projection on atomic wavefunctions
|
|
!
|
|
USE io_global, ONLY: stdout
|
|
USE mp_global, ONLY: intra_image_comm
|
|
USE mp, ONLY: mp_sum
|
|
USE electrons_base, ONLY: nx => nbspx, n => nbsp
|
|
USE gvecw, ONLY: ngw
|
|
USE reciprocal_vectors, ONLY: gstart
|
|
USE ions_base, ONLY: nsp, na, nas => nax, nat
|
|
USE uspp, ONLY: nhsa => nkb
|
|
USE atom, ONLY: nchi, lchi
|
|
!
|
|
IMPLICIT NONE
|
|
COMPLEX(8), INTENT(in) :: c(ngw,nx), eigr(ngw,nat), &
|
|
& betae(ngw,nhsa)
|
|
!
|
|
COMPLEX(8), ALLOCATABLE:: wfc(:,:), swfc(:,:), becwfc(:,:)
|
|
REAL(8), ALLOCATABLE :: overlap(:,:), e(:), z(:,:), &
|
|
& proj(:,:), temp(:)
|
|
REAL(8) :: somma
|
|
INTEGER n_atomic_wfc
|
|
INTEGER is, ia, nb, l, m, k, i
|
|
!
|
|
! calculate number of atomic states
|
|
!
|
|
n_atomic_wfc=0
|
|
DO is=1,nsp
|
|
DO nb = 1,nchi(is)
|
|
l = lchi(nb,is)
|
|
n_atomic_wfc = n_atomic_wfc + (2*l+1)*na(is)
|
|
END DO
|
|
END DO
|
|
IF (n_atomic_wfc.EQ.0) RETURN
|
|
!
|
|
ALLOCATE(wfc(ngw,n_atomic_wfc))
|
|
!
|
|
! calculate wfc = atomic states
|
|
!
|
|
CALL atomic_wfc(eigr,n_atomic_wfc,wfc)
|
|
!
|
|
! calculate bec = <beta|wfc>
|
|
!
|
|
ALLOCATE(becwfc(nhsa,n_atomic_wfc))
|
|
CALL nlsm1 (n_atomic_wfc,1,nsp,eigr,wfc,becwfc)
|
|
|
|
! calculate swfc = S|wfc>
|
|
!
|
|
ALLOCATE(swfc(ngw,n_atomic_wfc))
|
|
CALL s_wfc(n_atomic_wfc,becwfc,betae,wfc,swfc)
|
|
!
|
|
! calculate overlap(i,j) = <wfc_i|S|wfc_j>
|
|
!
|
|
ALLOCATE(overlap(n_atomic_wfc,n_atomic_wfc))
|
|
!
|
|
CALL MXMA(wfc,2*ngw,1,swfc,1,2*ngw,overlap,1, &
|
|
& n_atomic_wfc,n_atomic_wfc,2*ngw,n_atomic_wfc)
|
|
|
|
CALL mp_sum( overlap, intra_image_comm )
|
|
|
|
overlap=overlap*2.d0
|
|
IF (gstart == 2) THEN
|
|
DO l=1,n_atomic_wfc
|
|
DO m=1,n_atomic_wfc
|
|
overlap(m,l)=overlap(m,l)-DBLE(wfc(1,m))*DBLE(swfc(1,l))
|
|
END DO
|
|
END DO
|
|
END IF
|
|
!
|
|
! calculate (overlap)^(-1/2)(i,j). An orthonormal set of vectors |wfc_i>
|
|
! is obtained by introducing |wfc_j>=(overlap)^(-1/2)(i,j)*S|wfc_i>
|
|
!
|
|
ALLOCATE(z(n_atomic_wfc,n_atomic_wfc))
|
|
ALLOCATE(e(n_atomic_wfc))
|
|
CALL rdiag(n_atomic_wfc,overlap,n_atomic_wfc,e,z)
|
|
overlap=0.d0
|
|
DO l=1,n_atomic_wfc
|
|
DO m=1,n_atomic_wfc
|
|
DO k=1,n_atomic_wfc
|
|
overlap(l,m)=overlap(l,m)+z(m,k)*z(l,k)/SQRT(e(k))
|
|
END DO
|
|
END DO
|
|
END DO
|
|
DEALLOCATE(e)
|
|
DEALLOCATE(z)
|
|
!
|
|
! calculate |wfc_j>=(overlap)^(-1/2)(i,j)*S|wfc_i> (note the S matrix!)
|
|
!
|
|
wfc=0.d0
|
|
DO m=1,n_atomic_wfc
|
|
DO l=1,n_atomic_wfc
|
|
wfc(:,m)=wfc(:,m)+overlap(l,m)*swfc(:,l)
|
|
END DO
|
|
END DO
|
|
DEALLOCATE(overlap)
|
|
DEALLOCATE(swfc)
|
|
DEALLOCATE(becwfc)
|
|
!
|
|
! calculate proj = <c|S|wfc>
|
|
!
|
|
ALLOCATE(proj(n,n_atomic_wfc))
|
|
ALLOCATE(temp(ngw))
|
|
DO m=1,n
|
|
DO l=1,n_atomic_wfc
|
|
temp(:)=DBLE(CONJG(c(:,m))*wfc(:,l))
|
|
proj(m,l)=2.d0*SUM(temp)
|
|
IF (gstart == 2) proj(m,l)=proj(m,l)-temp(1)
|
|
END DO
|
|
END DO
|
|
DEALLOCATE(temp)
|
|
|
|
CALL mp_sum( proj, intra_image_comm )
|
|
|
|
i=0
|
|
WRITE( stdout,'(/''Projection on atomic states:'')')
|
|
DO is=1,nsp
|
|
DO nb = 1,nchi(is)
|
|
l=lchi(nb,is)
|
|
DO m = -l,l
|
|
DO ia=1,na(is)
|
|
i=i+1
|
|
WRITE( stdout,'(''atomic state # '',i3,'': atom # '',i3, &
|
|
& '' species # '',i2,'' wfc # '',i2, &
|
|
& '' (l='',i1,'' m='',i2,'')'')') &
|
|
& i, ia, is, nb, l, m
|
|
END DO
|
|
END DO
|
|
END DO
|
|
END DO
|
|
|
|
WRITE( stdout,*)
|
|
DO m=1,n
|
|
somma=0.d0
|
|
DO l=1,n_atomic_wfc
|
|
somma=somma+proj(m,l)**2
|
|
END DO
|
|
WRITE( stdout,'(''state # '',i4,'' sum c^2 ='',f7.4)') m,somma
|
|
WRITE( stdout,'(10f7.4)') (ABS(proj(m,l)),l=1,n_atomic_wfc)
|
|
END DO
|
|
!
|
|
DEALLOCATE(proj)
|
|
DEALLOCATE(wfc)
|
|
RETURN
|
|
END SUBROUTINE projwfc
|
|
!---------------------------------------------------------------------
|
|
SUBROUTINE randin(nmin,nmax,gstart,ngw,ampre,c)
|
|
!---------------------------------------------------------------------
|
|
!
|
|
USE wave_functions, ONLY: wave_rand_init
|
|
IMPLICIT NONE
|
|
|
|
! input
|
|
INTEGER nmin, nmax, gstart, ngw
|
|
REAL(8) ampre
|
|
! output
|
|
COMPLEX(8) c(ngw,nmax)
|
|
! local
|
|
INTEGER i,j
|
|
REAL(8) ranf1, randy, ranf2, ampexp
|
|
!
|
|
CALL wave_rand_init( c )
|
|
! do i=nmin,nmax
|
|
! do j=gstart,ngw
|
|
! ranf1=.5-randy()
|
|
! ranf2=.5-randy()
|
|
! ampexp=ampre*exp(-(4.*j)/ngw)
|
|
! c(j,i)=c(j,i)+ampexp*CMPLX(ranf1,ranf2)
|
|
! end do
|
|
! end do
|
|
!
|
|
RETURN
|
|
END SUBROUTINE randin
|
|
!
|
|
!-----------------------------------------------------------------------
|
|
SUBROUTINE rdiag (n,h,ldh,e,v)
|
|
!-----------------------------------------------------------------------
|
|
!
|
|
! calculates all the eigenvalues and eigenvectors of a complex
|
|
! hermitean matrix H . On output, the matrix H is destroyed
|
|
!
|
|
USE kinds, ONLY: DP
|
|
USE parallel_toolkit, ONLY: zhpev_drv
|
|
!
|
|
IMPLICIT NONE
|
|
!
|
|
INTEGER, INTENT(in) :: n, ldh
|
|
COMPLEX(DP), INTENT(inout):: h(ldh,n)
|
|
REAL (DP), INTENT(out) :: e(n)
|
|
COMPLEX(DP), INTENT(out) :: v(ldh,n)
|
|
!
|
|
INTEGER :: i, j, k
|
|
COMPLEX(DP), ALLOCATABLE :: ap( : )
|
|
!
|
|
ALLOCATE( ap( n * ( n + 1 ) / 2 ) )
|
|
|
|
K = 0
|
|
DO J = 1, n
|
|
DO I = J, n
|
|
K = K + 1
|
|
ap( k ) = h( i, j )
|
|
END DO
|
|
END DO
|
|
|
|
CALL zhpev_drv( 'V', 'L', n, ap, e, v, ldh )
|
|
|
|
DEALLOCATE( ap )
|
|
!
|
|
RETURN
|
|
END SUBROUTINE rdiag
|
|
|
|
!
|
|
!-----------------------------------------------------------------------
|
|
SUBROUTINE rhov(irb,eigrb,rhovan,rhog,rhor)
|
|
!-----------------------------------------------------------------------
|
|
! Add Vanderbilt contribution to rho(r) and rho(g)
|
|
!
|
|
! n_v(g) = sum_i,ij rho_i,ij q_i,ji(g) e^-ig.r_i
|
|
!
|
|
! routine makes use of c(-g)=c*(g) and beta(-g)=beta*(g)
|
|
!
|
|
USE kinds, ONLY: dp
|
|
USE ions_base, ONLY: nas => nax, nat, na, nsp
|
|
USE io_global, ONLY: stdout
|
|
USE mp_global, ONLY: intra_image_comm
|
|
USE mp, ONLY: mp_sum
|
|
USE cvan, ONLY: nvb
|
|
USE uspp_param, ONLY: nh, nhm
|
|
USE uspp, ONLY: deeq
|
|
USE grid_dimensions, ONLY: nr1, nr2, nr3, &
|
|
nr1x, nr2x, nr3x, nnr => nnrx
|
|
USE electrons_base, ONLY: nspin
|
|
USE gvecb
|
|
USE gvecp, ONLY: ng => ngm
|
|
USE cell_base, ONLY: omega
|
|
USE small_box, ONLY: omegab
|
|
USE smallbox_grid_dimensions, ONLY: nr1b, nr2b, nr3b, &
|
|
nr1bx, nr2bx, nr3bx, nnrb => nnrbx
|
|
USE control_flags, ONLY: iprint, iprsta
|
|
USE qgb_mod
|
|
USE recvecs_indexes, ONLY: np, nm
|
|
USE fft_module, ONLY: fwfft, invfft
|
|
USE fft_base, ONLY: dfftb
|
|
!
|
|
IMPLICIT NONE
|
|
!
|
|
REAL(8) :: rhovan(nhm*(nhm+1)/2,nat,nspin)
|
|
INTEGER, INTENT(in) :: irb(3,nat)
|
|
COMPLEX(8), INTENT(in):: eigrb(ngb,nat)
|
|
REAL(8), INTENT(inout):: rhor(nnr,nspin)
|
|
COMPLEX(8), INTENT(inout):: rhog(ng,nspin)
|
|
!
|
|
INTEGER isup, isdw, nfft, ifft, iv, jv, ig, ijv, is, iss, &
|
|
& isa, ia, ir
|
|
REAL(8) sumrho
|
|
COMPLEX(8) ci, fp, fm, ca
|
|
COMPLEX(8), ALLOCATABLE:: qgbt(:,:)
|
|
COMPLEX(8), ALLOCATABLE:: v(:)
|
|
COMPLEX(8), ALLOCATABLE:: qv(:)
|
|
!
|
|
IF (nvb.EQ.0) RETURN
|
|
CALL start_clock( 'rhov' )
|
|
ci=(0.,1.)
|
|
!
|
|
!
|
|
ALLOCATE( v( nnr ) )
|
|
ALLOCATE( qv( nnrb ) )
|
|
v (:) = (0.d0, 0.d0)
|
|
ALLOCATE( qgbt( ngb, 2 ) )
|
|
|
|
!
|
|
IF(nspin.EQ.1) THEN
|
|
!
|
|
! nspin=1 : two fft at a time, one per atom, if possible
|
|
!
|
|
iss=1
|
|
isa=1
|
|
|
|
DO is = 1, nvb
|
|
|
|
#ifdef __PARA
|
|
|
|
DO ia = 1, na(is)
|
|
nfft = 1
|
|
IF ( dfftb%np3( isa ) <= 0 ) go to 15
|
|
#else
|
|
|
|
DO ia = 1, na(is), 2
|
|
nfft = 2
|
|
#endif
|
|
|
|
IF( ia .EQ. na(is) ) nfft = 1
|
|
|
|
!
|
|
! nfft=2 if two ffts at the same time are performed
|
|
!
|
|
DO ifft=1,nfft
|
|
qgbt(:,ifft) = (0.d0, 0.d0)
|
|
DO iv= 1,nh(is)
|
|
DO jv=iv,nh(is)
|
|
ijv = (jv-1)*jv/2 + iv
|
|
sumrho=rhovan(ijv,isa+ifft-1,iss)
|
|
IF(iv.NE.jv) sumrho=2.*sumrho
|
|
DO ig=1,ngb
|
|
qgbt(ig,ifft)=qgbt(ig,ifft) + sumrho*qgb(ig,ijv,is)
|
|
END DO
|
|
END DO
|
|
END DO
|
|
END DO
|
|
!
|
|
! add structure factor
|
|
!
|
|
qv(:) = (0.d0, 0.d0)
|
|
IF(nfft.EQ.2)THEN
|
|
DO ig=1,ngb
|
|
qv(npb(ig))= &
|
|
eigrb(ig,isa )*qgbt(ig,1) &
|
|
+ ci* eigrb(ig,isa+1)*qgbt(ig,2)
|
|
qv(nmb(ig))= &
|
|
CONJG(eigrb(ig,isa )*qgbt(ig,1)) &
|
|
+ ci*CONJG(eigrb(ig,isa+1)*qgbt(ig,2))
|
|
END DO
|
|
ELSE
|
|
DO ig=1,ngb
|
|
qv(npb(ig)) = eigrb(ig,isa)*qgbt(ig,1)
|
|
qv(nmb(ig)) = CONJG(eigrb(ig,isa)*qgbt(ig,1))
|
|
END DO
|
|
ENDIF
|
|
|
|
CALL invfft('Box',qv,nr1b,nr2b,nr3b,nr1bx,nr2bx,nr3bx,isa)
|
|
|
|
!
|
|
! qv = US augmentation charge in real space on box grid
|
|
! for atomic species is, real(qv)=atom ia, imag(qv)=atom ia+1
|
|
|
|
IF(iprsta.GT.2) THEN
|
|
ca = SUM(qv)
|
|
WRITE( stdout,'(a,f12.8)') ' rhov: 1-atom g-sp = ', &
|
|
& omegab*DBLE(qgbt(1,1))
|
|
WRITE( stdout,'(a,f12.8)') ' rhov: 1-atom r-sp = ', &
|
|
& omegab*DBLE(ca)/(nr1b*nr2b*nr3b)
|
|
WRITE( stdout,'(a,f12.8)') ' rhov: 1-atom g-sp = ', &
|
|
& omegab*DBLE(qgbt(1,2))
|
|
WRITE( stdout,'(a,f12.8)') ' rhov: 1-atom r-sp = ', &
|
|
& omegab*AIMAG(ca)/(nr1b*nr2b*nr3b)
|
|
ENDIF
|
|
!
|
|
! add qv(r) to v(r), in real space on the dense grid
|
|
!
|
|
CALL box2grid(irb(1,isa),1,qv,v)
|
|
IF (nfft.EQ.2) CALL box2grid(irb(1,isa+1),2,qv,v)
|
|
15 isa=isa+nfft
|
|
!
|
|
END DO
|
|
END DO
|
|
!
|
|
! rhor(r) = total (smooth + US) charge density in real space
|
|
!
|
|
DO ir=1,nnr
|
|
rhor(ir,iss)=rhor(ir,iss)+DBLE(v(ir))
|
|
END DO
|
|
!
|
|
IF(iprsta.GT.2) THEN
|
|
ca = SUM(v)
|
|
|
|
CALL mp_sum( ca, intra_image_comm )
|
|
|
|
WRITE( stdout,'(a,2f12.8)') &
|
|
& ' rhov: int n_v(r) dr = ',omega*ca/(nr1*nr2*nr3)
|
|
ENDIF
|
|
!
|
|
CALL fwfft('Dense',v,nr1,nr2,nr3,nr1x,nr2x,nr3x)
|
|
!
|
|
IF(iprsta.GT.2) THEN
|
|
WRITE( stdout,*) ' rhov: smooth ',omega*rhog(1,iss)
|
|
WRITE( stdout,*) ' rhov: vander ',omega*v(1)
|
|
WRITE( stdout,*) ' rhov: all ',omega*(rhog(1,iss)+v(1))
|
|
ENDIF
|
|
!
|
|
! rhog(g) = total (smooth + US) charge density in G-space
|
|
!
|
|
DO ig=1,ng
|
|
rhog(ig,iss)=rhog(ig,iss)+v(np(ig))
|
|
END DO
|
|
!
|
|
IF(iprsta.GT.1) WRITE( stdout,'(a,2f12.8)') &
|
|
& ' rhov: n_v(g=0) = ',omega*DBLE(rhog(1,iss))
|
|
!
|
|
ELSE
|
|
!
|
|
! nspin=2: two fft at a time, one for spin up and one for spin down
|
|
!
|
|
isup=1
|
|
isdw=2
|
|
isa=1
|
|
DO is=1,nvb
|
|
DO ia=1,na(is)
|
|
#ifdef __PARA
|
|
IF ( dfftb%np3( isa ) <= 0 ) go to 25
|
|
#endif
|
|
DO iss=1,2
|
|
qgbt(:,iss) = (0.d0, 0.d0)
|
|
DO iv=1,nh(is)
|
|
DO jv=iv,nh(is)
|
|
ijv = (jv-1)*jv/2 + iv
|
|
sumrho=rhovan(ijv,isa,iss)
|
|
IF(iv.NE.jv) sumrho=2.*sumrho
|
|
DO ig=1,ngb
|
|
qgbt(ig,iss)=qgbt(ig,iss)+sumrho*qgb(ig,ijv,is)
|
|
END DO
|
|
END DO
|
|
END DO
|
|
END DO
|
|
!
|
|
! add structure factor
|
|
!
|
|
qv(:) = (0.d0, 0.d0)
|
|
DO ig=1,ngb
|
|
qv(npb(ig)) = eigrb(ig,isa)*qgbt(ig,1) &
|
|
& + ci* eigrb(ig,isa)*qgbt(ig,2)
|
|
qv(nmb(ig)) = CONJG(eigrb(ig,isa)*qgbt(ig,1)) &
|
|
& + ci* CONJG(eigrb(ig,isa)*qgbt(ig,2))
|
|
END DO
|
|
!
|
|
CALL invfft('Box',qv,nr1b,nr2b,nr3b,nr1bx,nr2bx,nr3bx,isa)
|
|
!
|
|
! qv is the now the US augmentation charge for atomic species is
|
|
! and atom ia: real(qv)=spin up, imag(qv)=spin down
|
|
!
|
|
IF(iprsta.GT.2) THEN
|
|
ca = SUM(qv)
|
|
WRITE( stdout,'(a,f12.8)') ' rhov: up g-space = ', &
|
|
& omegab*DBLE(qgbt(1,1))
|
|
WRITE( stdout,'(a,f12.8)') ' rhov: up r-sp = ', &
|
|
& omegab*DBLE(ca)/(nr1b*nr2b*nr3b)
|
|
WRITE( stdout,'(a,f12.8)') ' rhov: dw g-space = ', &
|
|
& omegab*DBLE(qgbt(1,2))
|
|
WRITE( stdout,'(a,f12.8)') ' rhov: dw r-sp = ', &
|
|
& omegab*AIMAG(ca)/(nr1b*nr2b*nr3b)
|
|
ENDIF
|
|
!
|
|
! add qv(r) to v(r), in real space on the dense grid
|
|
!
|
|
CALL box2grid2(irb(1,isa),qv,v)
|
|
25 isa=isa+1
|
|
!
|
|
END DO
|
|
END DO
|
|
!
|
|
DO ir=1,nnr
|
|
rhor(ir,isup)=rhor(ir,isup)+DBLE(v(ir))
|
|
rhor(ir,isdw)=rhor(ir,isdw)+AIMAG(v(ir))
|
|
END DO
|
|
!
|
|
IF(iprsta.GT.2) THEN
|
|
ca = SUM(v)
|
|
CALL mp_sum( ca, intra_image_comm )
|
|
WRITE( stdout,'(a,2f12.8)') 'rhov:in n_v ',omega*ca/(nr1*nr2*nr3)
|
|
ENDIF
|
|
!
|
|
CALL fwfft('Dense',v,nr1,nr2,nr3,nr1x,nr2x,nr3x)
|
|
!
|
|
IF(iprsta.GT.2) THEN
|
|
WRITE( stdout,*) 'rhov: smooth up',omega*rhog(1,isup)
|
|
WRITE( stdout,*) 'rhov: smooth dw',omega*rhog(1,isdw)
|
|
WRITE( stdout,*) 'rhov: vander up',omega*DBLE(v(1))
|
|
WRITE( stdout,*) 'rhov: vander dw',omega*AIMAG(v(1))
|
|
WRITE( stdout,*) 'rhov: all up', &
|
|
& omega*(rhog(1,isup)+DBLE(v(1)))
|
|
WRITE( stdout,*) 'rhov: all dw', &
|
|
& omega*(rhog(1,isdw)+AIMAG(v(1)))
|
|
ENDIF
|
|
!
|
|
DO ig=1,ng
|
|
fp= v(np(ig)) + v(nm(ig))
|
|
fm= v(np(ig)) - v(nm(ig))
|
|
rhog(ig,isup)=rhog(ig,isup) + 0.5*CMPLX(DBLE(fp),AIMAG(fm))
|
|
rhog(ig,isdw)=rhog(ig,isdw) + 0.5*CMPLX(AIMAG(fp),-DBLE(fm))
|
|
END DO
|
|
!
|
|
IF(iprsta.GT.2) WRITE( stdout,'(a,2f12.8)') &
|
|
& ' rhov: n_v(g=0) up = ',omega*DBLE (rhog(1,isup))
|
|
IF(iprsta.GT.2) WRITE( stdout,'(a,2f12.8)') &
|
|
& ' rhov: n_v(g=0) down = ',omega*DBLE(rhog(1,isdw))
|
|
!
|
|
ENDIF
|
|
|
|
DEALLOCATE(qgbt)
|
|
DEALLOCATE( v )
|
|
DEALLOCATE( qv )
|
|
|
|
CALL stop_clock( 'rhov' )
|
|
!
|
|
RETURN
|
|
END SUBROUTINE rhov
|
|
!
|
|
!
|
|
!-------------------------------------------------------------------------
|
|
SUBROUTINE s_wfc(n_atomic_wfc,becwfc,betae,wfc,swfc)
|
|
!-----------------------------------------------------------------------
|
|
!
|
|
! input: wfc, becwfc=<wfc|beta>, betae=|beta>
|
|
! output: swfc=S|wfc>
|
|
!
|
|
USE ions_base, ONLY: na
|
|
USE cvan, ONLY: nvb, ish
|
|
USE uspp, ONLY: nhsa => nkb, nhsavb=>nkbus, qq
|
|
USE uspp_param, ONLY: nh
|
|
USE gvecw, ONLY: ngw
|
|
!use parm
|
|
USE constants, ONLY: pi, fpi
|
|
IMPLICIT NONE
|
|
! input
|
|
INTEGER, INTENT(in) :: n_atomic_wfc
|
|
COMPLEX(8), INTENT(in) :: betae(ngw,nhsa), &
|
|
& wfc(ngw,n_atomic_wfc)
|
|
REAL(8), INTENT(in) :: becwfc(nhsa,n_atomic_wfc)
|
|
! output
|
|
COMPLEX(8), INTENT(out):: swfc(ngw,n_atomic_wfc)
|
|
! local
|
|
INTEGER is, iv, jv, ia, inl, jnl, i
|
|
REAL(8) qtemp(nhsavb,n_atomic_wfc)
|
|
!
|
|
swfc=0.d0
|
|
!
|
|
IF (nvb.GT.0) THEN
|
|
qtemp=0.d0
|
|
DO is=1,nvb
|
|
DO iv=1,nh(is)
|
|
DO jv=1,nh(is)
|
|
IF(ABS(qq(iv,jv,is)).GT.1.e-5) THEN
|
|
DO ia=1,na(is)
|
|
inl=ish(is)+(iv-1)*na(is)+ia
|
|
jnl=ish(is)+(jv-1)*na(is)+ia
|
|
DO i=1,n_atomic_wfc
|
|
qtemp(inl,i) = qtemp(inl,i) + &
|
|
& qq(iv,jv,is)*becwfc(jnl,i)
|
|
END DO
|
|
END DO
|
|
ENDIF
|
|
END DO
|
|
END DO
|
|
END DO
|
|
!
|
|
CALL MXMA (betae,1,2*ngw,qtemp,1,nhsavb,swfc,1, &
|
|
& 2*ngw,2*ngw,nhsavb,n_atomic_wfc)
|
|
END IF
|
|
!
|
|
swfc=swfc+wfc
|
|
!
|
|
RETURN
|
|
END SUBROUTINE s_wfc
|
|
|
|
!-----------------------------------------------------------------------
|
|
SUBROUTINE spinsq (c,bec,rhor)
|
|
!-----------------------------------------------------------------------
|
|
!
|
|
! estimate of <S^2>=s(s+1) in two different ways.
|
|
! 1) using as many-body wavefunction a single Slater determinant
|
|
! constructed with Kohn-Sham orbitals:
|
|
!
|
|
! <S^2> = (Nup-Ndw)/2 * (Nup-Ndw)/2+1) + Ndw -
|
|
! \sum_up\sum_dw < psi_up | psi_dw >
|
|
!
|
|
! where Nup, Ndw = number of up and down states, the sum is over
|
|
! occupied states. Not suitable for fractionary occupancy.
|
|
! In the ultrasoft scheme (c is the smooth part of \psi):
|
|
!
|
|
! < psi_up | psi_dw > = \sum_G c*_up(G) c_dw(G) +
|
|
! \int Q_ij <c_up|beta_i><beta_j|c_dw>
|
|
!
|
|
! This is the usual formula, unsuitable for fractionary occupancy.
|
|
! 2) using the "LSD model" of Wang, Becke, Smith, JCP 102, 3477 (1995):
|
|
!
|
|
! <S^2> = (Nup-Ndw)/2 * (Nup-Ndw)/2+1) + Ndw -
|
|
! \int max(rhoup(r),rhodw(r)) dr
|
|
!
|
|
! Requires on input: c=psi, bec=<c|beta>, rhoup(r), rhodw(r)
|
|
! Assumes real psi, with only half G vectors.
|
|
!
|
|
USE electrons_base, ONLY: nx => nbspx, n => nbsp, iupdwn, nupdwn, f, nel, nspin
|
|
USE io_global, ONLY: stdout
|
|
USE mp_global, ONLY: intra_image_comm
|
|
USE mp, ONLY: mp_sum
|
|
USE gvecw, ONLY: ngw
|
|
USE reciprocal_vectors, ONLY: gstart
|
|
USE grid_dimensions, ONLY: nr1, nr2, nr3, &
|
|
nnr => nnrx
|
|
USE cell_base, ONLY: omega
|
|
USE cvan, ONLY: nvb, ish
|
|
USE uspp, ONLY: nhsa => nkb, nhsavb=>nkbus, qq
|
|
USE uspp_param, ONLY: nh
|
|
USE ions_base, ONLY: na
|
|
!
|
|
IMPLICIT NONE
|
|
! input
|
|
REAL(8) bec(nhsa,n), rhor(nnr,nspin)
|
|
COMPLEX(8) c(ngw,nx)
|
|
! local variables
|
|
INTEGER nup, ndw, ir, i, j, jj, ig, ia, is, iv, jv, inl, jnl
|
|
REAL(8) spin0, spin1, spin2, fup, fdw
|
|
REAL(8), ALLOCATABLE:: overlap(:,:), temp(:)
|
|
LOGICAL frac
|
|
!
|
|
!
|
|
IF (nspin.EQ.1) RETURN
|
|
!
|
|
! find spin-up and spin-down states
|
|
!
|
|
fup = 0.0
|
|
DO i=iupdwn(1),nupdwn(1)
|
|
fup = fup + f(i)
|
|
END DO
|
|
nup = NINT(fup)
|
|
ndw = nel(1)+nel(2) - nup
|
|
!
|
|
! paranoid checks
|
|
!
|
|
frac= ABS(fup-nup).GT.1.0e-6
|
|
fup = 0.0
|
|
DO i=1,nup
|
|
fup = fup + f(i)
|
|
END DO
|
|
frac=frac.OR.ABS(fup-nup).GT.1.0e-6
|
|
fdw = 0.0
|
|
DO j=iupdwn(2),iupdwn(2)-1+ndw
|
|
fdw = fdw + f(j)
|
|
END DO
|
|
frac=frac.OR.ABS(fdw-ndw).GT.1.0e-6
|
|
!
|
|
spin0 = ABS(fup-fdw)/2.d0 * ( ABS(fup-fdw)/2.d0 + 1.d0 ) + fdw
|
|
!
|
|
! Becke's formula for spin polarization
|
|
!
|
|
spin1 = 0.0
|
|
DO ir=1,nnr
|
|
spin1 = spin1 - MIN(rhor(ir,1),rhor(ir,2))
|
|
END DO
|
|
CALL mp_sum( spin1, intra_image_comm )
|
|
spin1 = spin0 + omega/(nr1*nr2*nr3)*spin1
|
|
IF (frac) THEN
|
|
WRITE( stdout,'(/'' Spin contamination: s(s+1)='',f5.2,'' (Becke) '',&
|
|
& f5.2,'' (expected)'')') &
|
|
& spin1, ABS(fup-fdw)/2.d0*(ABS(fup-fdw)/2.d0+1.d0)
|
|
RETURN
|
|
END IF
|
|
!
|
|
! Slater formula, smooth contribution to < psi_up | psi_dw >
|
|
!
|
|
ALLOCATE (overlap(nup,ndw))
|
|
ALLOCATE (temp(ngw))
|
|
DO j=1,ndw
|
|
jj=j+iupdwn(2)-1
|
|
DO i=1,nup
|
|
overlap(i,j)=0.d0
|
|
DO ig=1,ngw
|
|
temp(ig)=DBLE(CONJG(c(ig,i))*c(ig,jj))
|
|
END DO
|
|
overlap(i,j) = 2.d0*SUM(temp)
|
|
IF (gstart == 2) overlap(i,j) = overlap(i,j) - temp(1)
|
|
END DO
|
|
END DO
|
|
DEALLOCATE (temp)
|
|
CALL mp_sum( overlap, intra_image_comm )
|
|
DO j=1,ndw
|
|
jj=j+iupdwn(2)-1
|
|
DO i=1,nup
|
|
!
|
|
! vanderbilt contribution to < psi_up | psi_dw >
|
|
!
|
|
DO is=1,nvb
|
|
DO iv=1,nh(is)
|
|
DO jv=1,nh(is)
|
|
IF(ABS(qq(iv,jv,is)).GT.1.e-5) THEN
|
|
DO ia=1,na(is)
|
|
inl=ish(is)+(iv-1)*na(is)+ia
|
|
jnl=ish(is)+(jv-1)*na(is)+ia
|
|
overlap(i,j) = overlap(i,j) + &
|
|
& qq(iv,jv,is)*bec(inl,i)*bec(jnl,jj)
|
|
END DO
|
|
ENDIF
|
|
END DO
|
|
END DO
|
|
END DO
|
|
END DO
|
|
END DO
|
|
!
|
|
spin2 = spin0
|
|
DO j=1,ndw
|
|
DO i=1,nup
|
|
spin2 = spin2 - overlap(i,j)**2
|
|
END DO
|
|
END DO
|
|
!
|
|
DEALLOCATE (overlap)
|
|
!
|
|
WRITE( stdout,'(/" Spin contamination: s(s+1)=",f5.2," (Slater) ", &
|
|
& f5.2," (Becke) ",f5.2," (expected)")') &
|
|
& spin2,spin1, ABS(fup-fdw)/2.d0*(ABS(fup-fdw)/2.d0+1.d0)
|
|
!
|
|
RETURN
|
|
END SUBROUTINE spinsq
|
|
|
|
!
|
|
!-----------------------------------------------------------------------
|
|
SUBROUTINE vofrho( nfi, rhor, rhog, rhos, rhoc, tfirst, tlast, &
|
|
& ei1, ei2, ei3, irb, eigrb, sfac, tau0, fion )
|
|
!-----------------------------------------------------------------------
|
|
! computes: the one-particle potential v in real space,
|
|
! the total energy etot,
|
|
! the forces fion acting on the ions,
|
|
! the derivative of total energy to cell parameters h
|
|
! rhor input : electronic charge on dense real space grid
|
|
! (plus core charge if present)
|
|
! rhog input : electronic charge in g space (up to density cutoff)
|
|
! rhos input : electronic charge on smooth real space grid
|
|
! rhor output: total potential on dense real space grid
|
|
! rhos output: total potential on smooth real space grid
|
|
!
|
|
USE kinds, ONLY: dp
|
|
USE control_flags, ONLY: iprint, iprsta, thdyn, tpre, tfor, tprnfor
|
|
USE io_global, ONLY: stdout
|
|
USE ions_base, ONLY: nas => nax, nsp, na, nat
|
|
USE gvecs
|
|
USE gvecp, ONLY: ng => ngm
|
|
USE cell_base, ONLY: omega
|
|
USE cell_base, ONLY: a1, a2, a3, tpiba2
|
|
USE reciprocal_vectors, ONLY: gstart, g
|
|
USE recvecs_indexes, ONLY: np, nm
|
|
USE grid_dimensions, ONLY: nr1, nr2, nr3, &
|
|
nr1x, nr2x, nr3x, nnr => nnrx
|
|
USE smooth_grid_dimensions, ONLY: nr1s, nr2s, nr3s, &
|
|
nr1sx, nr2sx, nr3sx, nnrsx
|
|
USE electrons_base, ONLY: nspin
|
|
USE constants, ONLY: pi, fpi
|
|
USE energies, ONLY: etot, eself, enl, ekin, epseu, esr, eht, exc
|
|
USE local_pseudo, ONLY: vps, rhops
|
|
USE core, ONLY: nlcc_any
|
|
USE gvecb
|
|
USE dener
|
|
USE derho
|
|
USE mp, ONLY: mp_sum
|
|
USE mp_global, ONLY: intra_image_comm
|
|
USE funct, ONLY: dft_is_meta
|
|
USE fft_module, ONLY: fwfft, invfft
|
|
USE sic_module, ONLY: self_interaction, sic_epsilon, sic_alpha
|
|
USE energies, ONLY: self_sxc, self_ehte
|
|
!
|
|
IMPLICIT NONE
|
|
!
|
|
LOGICAL :: tlast, tfirst
|
|
INTEGER :: nfi
|
|
REAL(DP) rhor(nnr,nspin), rhos(nnrsx,nspin), fion(3,nat)
|
|
REAL(DP) rhoc(nnr), tau0(3,nat)
|
|
COMPLEX(DP) ei1(-nr1:nr1,nat), ei2(-nr2:nr2,nat), &
|
|
& ei3(-nr3:nr3,nat), eigrb(ngb,nat), &
|
|
& rhog(ng,nspin), sfac(ngs,nsp)
|
|
!
|
|
INTEGER irb(3,nat), iss, isup, isdw, ig, ir,i,j,k,is, ia
|
|
REAL(DP) fion1(3,nat), vave, ebac, wz, eh
|
|
COMPLEX(DP) fp, fm, ci
|
|
COMPLEX(DP), ALLOCATABLE :: v(:), vs(:)
|
|
COMPLEX(DP), ALLOCATABLE :: rhotmp(:), vtemp(:), drhotmp(:,:,:)
|
|
!
|
|
COMPLEX(DP), ALLOCATABLE :: self_vloc(:)
|
|
COMPLEX(DP) :: self_rhoeg
|
|
REAL(DP) :: self_ehtet , fpibg
|
|
LOGICAL :: ttsic
|
|
!
|
|
|
|
CALL start_clock( 'vofrho' )
|
|
ci=(0.,1.)
|
|
!
|
|
! wz = factor for g.neq.0 because of c*(g)=c(-g)
|
|
!
|
|
wz = 2.0
|
|
ALLOCATE( v( nnr ) )
|
|
ALLOCATE( vs( nnrsx ) )
|
|
ALLOCATE(vtemp(ng))
|
|
ALLOCATE(rhotmp(ng))
|
|
IF (tpre) ALLOCATE(drhotmp(ng,3,3))
|
|
!
|
|
ttsic = ( ABS(self_interaction) /= 0 )
|
|
IF( tpre .AND. ttsic ) &
|
|
& CALL errore('in cplib tpre and ttsic are not possible', 1)
|
|
|
|
IF( ttsic ) ALLOCATE(self_vloc(ng))
|
|
!
|
|
! first routine in which fion is calculated: annihilation
|
|
!
|
|
fion =0.d0
|
|
fion1=0.d0
|
|
!
|
|
! ===================================================================
|
|
! forces on ions, ionic term in real space
|
|
! -------------------------------------------------------------------
|
|
IF( tprnfor .OR. tfor .OR. tfirst .OR. tpre ) THEN
|
|
CALL force_ion( tau0, esr, fion, dsr )
|
|
END IF
|
|
!
|
|
|
|
IF( nspin == 1 ) THEN
|
|
iss=1
|
|
DO ig=1,ng
|
|
rhotmp(ig)=rhog(ig,iss)
|
|
END DO
|
|
IF(tpre)THEN
|
|
DO j=1,3
|
|
DO i=1,3
|
|
DO ig=1,ng
|
|
drhotmp(ig,i,j)=drhog(ig,iss,i,j)
|
|
ENDDO
|
|
ENDDO
|
|
ENDDO
|
|
ENDIF
|
|
ELSE
|
|
isup=1
|
|
isdw=2
|
|
DO ig=1,ng
|
|
rhotmp(ig)=rhog(ig,isup)+rhog(ig,isdw)
|
|
END DO
|
|
IF(tpre)THEN
|
|
DO i=1,3
|
|
DO j=1,3
|
|
DO ig=1,ng
|
|
drhotmp(ig,i,j) = drhog(ig,isup,i,j) + &
|
|
& drhog(ig,isdw,i,j)
|
|
ENDDO
|
|
ENDDO
|
|
ENDDO
|
|
ENDIF
|
|
END IF
|
|
! ===================================================================
|
|
! calculation local potential energy
|
|
! -------------------------------------------------------------------
|
|
vtemp=(0.,0.)
|
|
DO is=1,nsp
|
|
DO ig=1,ngs
|
|
vtemp(ig)=vtemp(ig)+CONJG(rhotmp(ig))*sfac(ig,is)*vps(ig,is)
|
|
END DO
|
|
END DO
|
|
|
|
epseu=wz*DBLE(SUM(vtemp))
|
|
IF (gstart == 2) epseu=epseu-vtemp(1)
|
|
CALL mp_sum( epseu, intra_image_comm )
|
|
epseu=epseu*omega
|
|
!
|
|
IF(tpre) CALL denps(rhotmp,drhotmp,sfac,vtemp,dps)
|
|
!
|
|
! ===================================================================
|
|
! calculation hartree energy
|
|
! -------------------------------------------------------------------
|
|
!
|
|
self_ehtet = 0.d0
|
|
IF( ALLOCATED( self_vloc ) ) self_vloc = 0.d0
|
|
|
|
DO is=1,nsp
|
|
DO ig=1,ngs
|
|
rhotmp(ig)=rhotmp(ig)+sfac(ig,is)*rhops(ig,is)
|
|
END DO
|
|
END DO
|
|
IF (gstart == 2) vtemp(1)=0.0
|
|
DO ig=gstart,ng
|
|
vtemp(ig)=CONJG(rhotmp(ig))*rhotmp(ig)/g(ig)
|
|
END DO
|
|
!
|
|
eh=DBLE(SUM(vtemp))*wz*0.5*fpi/tpiba2
|
|
!
|
|
IF ( ttsic ) THEN
|
|
DO ig = gstart,ng
|
|
!
|
|
fpibg = fpi /(tpiba2 *g(ig))
|
|
!
|
|
self_rhoeg = rhog(ig,1) - rhog(ig,2)
|
|
self_ehtet = self_ehtet + fpibg * DBLE(self_rhoeg * CONJG(self_rhoeg))
|
|
self_vloc(ig) = sic_epsilon * fpibg * self_rhoeg
|
|
!
|
|
ENDDO
|
|
|
|
IF(gstart == 2) self_vloc(1) = 0.D0
|
|
self_ehte = sic_epsilon * self_ehtet * wz * 0.5d0
|
|
eh = eh - self_ehte
|
|
|
|
CALL mp_sum( self_ehte, intra_image_comm )
|
|
|
|
ENDIF
|
|
!
|
|
CALL mp_sum( eh, intra_image_comm )
|
|
!
|
|
IF(tpre) CALL denh(rhotmp,drhotmp,sfac,vtemp,eh,dh)
|
|
IF(tpre) DEALLOCATE(drhotmp)
|
|
|
|
! ===================================================================
|
|
! forces on ions, ionic term in reciprocal space
|
|
! -------------------------------------------------------------------
|
|
IF( tprnfor .OR. tfor .OR. tpre) &
|
|
& CALL force_ps(rhotmp,rhog,vtemp,ei1,ei2,ei3,fion1)
|
|
! ===================================================================
|
|
! calculation hartree + local pseudo potential
|
|
! -------------------------------------------------------------------
|
|
!
|
|
IF (gstart == 2) vtemp(1)=(0.,0.)
|
|
DO ig=gstart,ng
|
|
vtemp(ig)=rhotmp(ig)*fpi/(tpiba2*g(ig))
|
|
END DO
|
|
!
|
|
DO is=1,nsp
|
|
DO ig=1,ngs
|
|
vtemp(ig)=vtemp(ig)+sfac(ig,is)*vps(ig,is)
|
|
END DO
|
|
END DO
|
|
!
|
|
! vtemp = v_loc(g) + v_h(g)
|
|
!
|
|
! ===================================================================
|
|
! calculation exchange and correlation energy and potential
|
|
! -------------------------------------------------------------------
|
|
IF (nlcc_any) CALL add_cc(rhoc,rhog,rhor)
|
|
!
|
|
CALL exch_corr_h( nspin, rhog, rhor, rhoc, sfac, exc, dxc, self_sxc )
|
|
|
|
!
|
|
! rhor contains the xc potential in r-space
|
|
!
|
|
! ===================================================================
|
|
! fourier transform of xc potential to g-space (dense grid)
|
|
! -------------------------------------------------------------------
|
|
!
|
|
IF( nspin == 1 ) THEN
|
|
iss = 1
|
|
DO ir = 1, nnr
|
|
v(ir) = CMPLX( rhor( ir, iss ), 0.d0 )
|
|
END DO
|
|
!
|
|
! v_xc(r) --> v_xc(g)
|
|
!
|
|
CALL fwfft( 'Dense', v, nr1, nr2, nr3, nr1x, nr2x, nr3x )
|
|
!
|
|
DO ig = 1, ng
|
|
rhog( ig, iss ) = vtemp(ig) + v( np( ig ) )
|
|
END DO
|
|
!
|
|
! v_tot(g) = (v_tot(g) - v_xc(g)) +v_xc(g)
|
|
! rhog contains the total potential in g-space
|
|
!
|
|
ELSE
|
|
isup=1
|
|
isdw=2
|
|
DO ir=1,nnr
|
|
v(ir)=CMPLX(rhor(ir,isup),rhor(ir,isdw))
|
|
END DO
|
|
CALL fwfft('Dense',v,nr1,nr2,nr3,nr1x,nr2x,nr3x)
|
|
DO ig=1,ng
|
|
fp=v(np(ig))+v(nm(ig))
|
|
fm=v(np(ig))-v(nm(ig))
|
|
IF( ttsic ) THEN
|
|
rhog(ig,isup)=vtemp(ig)-self_vloc(ig) +0.5*CMPLX( DBLE(fp),AIMAG(fm))
|
|
rhog(ig,isdw)=vtemp(ig)+self_vloc(ig) +0.5*CMPLX(AIMAG(fp),-DBLE(fm))
|
|
ELSE
|
|
rhog(ig,isup)=vtemp(ig)+0.5*CMPLX( DBLE(fp),AIMAG(fm))
|
|
rhog(ig,isdw)=vtemp(ig)+0.5*CMPLX(AIMAG(fp),-DBLE(fm))
|
|
ENDIF
|
|
END DO
|
|
ENDIF
|
|
|
|
!
|
|
! rhog contains now the total (local+Hartree+xc) potential in g-space
|
|
!
|
|
IF( tprnfor .OR. tfor ) THEN
|
|
|
|
IF ( nlcc_any ) CALL force_cc( irb, eigrb, rhor, fion1 )
|
|
|
|
CALL mp_sum( fion1, intra_image_comm )
|
|
!
|
|
! add g-space ionic and core correction contributions to fion
|
|
!
|
|
fion = fion + fion1
|
|
|
|
END IF
|
|
!
|
|
IF( ALLOCATED( self_vloc ) ) DEALLOCATE( self_vloc )
|
|
!
|
|
! ===================================================================
|
|
! fourier transform of total potential to r-space (dense grid)
|
|
! -------------------------------------------------------------------
|
|
v(:) = (0.d0, 0.d0)
|
|
IF(nspin.EQ.1) THEN
|
|
iss=1
|
|
DO ig=1,ng
|
|
v(np(ig))=rhog(ig,iss)
|
|
v(nm(ig))=CONJG(rhog(ig,iss))
|
|
END DO
|
|
!
|
|
! v(g) --> v(r)
|
|
!
|
|
CALL invfft('Dense',v,nr1,nr2,nr3,nr1x,nr2x,nr3x)
|
|
!
|
|
DO ir=1,nnr
|
|
rhor(ir,iss)=DBLE(v(ir))
|
|
END DO
|
|
!
|
|
! calculation of average potential
|
|
!
|
|
vave=SUM(rhor(:,iss))/DBLE(nr1*nr2*nr3)
|
|
ELSE
|
|
isup=1
|
|
isdw=2
|
|
DO ig=1,ng
|
|
v(np(ig))=rhog(ig,isup)+ci*rhog(ig,isdw)
|
|
v(nm(ig))=CONJG(rhog(ig,isup)) +ci*CONJG(rhog(ig,isdw))
|
|
END DO
|
|
!
|
|
CALL invfft('Dense',v,nr1,nr2,nr3,nr1x,nr2x,nr3x)
|
|
DO ir=1,nnr
|
|
rhor(ir,isup)= DBLE(v(ir))
|
|
rhor(ir,isdw)=AIMAG(v(ir))
|
|
END DO
|
|
!
|
|
! calculation of average potential
|
|
!
|
|
vave=(SUM(rhor(:,isup))+SUM(rhor(:,isdw))) &
|
|
& /2.0/DBLE(nr1*nr2*nr3)
|
|
ENDIF
|
|
|
|
CALL mp_sum( vave, intra_image_comm )
|
|
|
|
!
|
|
! fourier transform of total potential to r-space (smooth grid)
|
|
!
|
|
vs (:) = (0.d0, 0.d0)
|
|
!
|
|
IF(nspin.EQ.1)THEN
|
|
iss=1
|
|
DO ig=1,ngs
|
|
vs(nms(ig))=CONJG(rhog(ig,iss))
|
|
vs(nps(ig))=rhog(ig,iss)
|
|
END DO
|
|
!
|
|
CALL invfft('Smooth',vs,nr1s,nr2s,nr3s,nr1sx,nr2sx,nr3sx)
|
|
!
|
|
DO ir=1,nnrsx
|
|
rhos(ir,iss)=DBLE(vs(ir))
|
|
END DO
|
|
ELSE
|
|
isup=1
|
|
isdw=2
|
|
DO ig=1,ngs
|
|
vs(nps(ig))=rhog(ig,isup)+ci*rhog(ig,isdw)
|
|
vs(nms(ig))=CONJG(rhog(ig,isup)) +ci*CONJG(rhog(ig,isdw))
|
|
END DO
|
|
CALL invfft('Smooth',vs,nr1s,nr2s,nr3s,nr1sx,nr2sx,nr3sx)
|
|
DO ir=1,nnrsx
|
|
rhos(ir,isup)= DBLE(vs(ir))
|
|
rhos(ir,isdw)=AIMAG(vs(ir))
|
|
END DO
|
|
ENDIF
|
|
|
|
IF( dft_is_meta() ) CALL vofrho_meta( v, vs ) !METAGGA
|
|
|
|
ebac=0.0
|
|
!
|
|
eht=eh*omega+esr-eself
|
|
!
|
|
! etot is the total energy ; ekin, enl were calculated in rhoofr
|
|
!
|
|
etot=ekin+eht+epseu+enl+exc+ebac
|
|
IF(tpre) detot=dekin+dh+dps+denl+dxc+dsr
|
|
!
|
|
DEALLOCATE(rhotmp)
|
|
DEALLOCATE(vtemp)
|
|
DEALLOCATE( v )
|
|
DEALLOCATE( vs )
|
|
!
|
|
CALL stop_clock( 'vofrho' )
|
|
|
|
IF( ( nfi == 0 ) .OR. tfirst .OR. tlast ) GOTO 999
|
|
IF( MOD( nfi - 1, iprint) /= 0 ) RETURN
|
|
!
|
|
999 IF ( tpre ) THEN
|
|
IF( iprsta >= 2 ) THEN
|
|
WRITE( stdout,*)
|
|
WRITE( stdout,*) "From vofrho:"
|
|
WRITE( stdout,*) "cell parameters h"
|
|
WRITE( stdout,5555) (a1(i),a2(i),a3(i),i=1,3)
|
|
WRITE( stdout,*)
|
|
WRITE( stdout,*) "derivative of e(tot)"
|
|
WRITE( stdout,5555) ((detot(i,j),j=1,3),i=1,3)
|
|
WRITE( stdout,*)
|
|
WRITE( stdout,*) "derivative of e(kin)"
|
|
WRITE( stdout,5555) ((dekin(i,j),j=1,3),i=1,3)
|
|
WRITE( stdout,*) "derivative of e(electrostatic)"
|
|
WRITE( stdout,5555) (((dh(i,j)+dsr(i,j)),j=1,3),i=1,3)
|
|
WRITE( stdout,*) "derivative of e(h)"
|
|
WRITE( stdout,5555) ((dh(i,j),j=1,3),i=1,3)
|
|
WRITE( stdout,*) "derivative of e(sr)"
|
|
WRITE( stdout,5555) ((dsr(i,j),j=1,3),i=1,3)
|
|
WRITE( stdout,*) "derivative of e(ps)"
|
|
WRITE( stdout,5555) ((dps(i,j),j=1,3),i=1,3)
|
|
WRITE( stdout,*) "derivative of e(nl)"
|
|
WRITE( stdout,5555) ((denl(i,j),j=1,3),i=1,3)
|
|
WRITE( stdout,*) "derivative of e(xc)"
|
|
WRITE( stdout,5555) ((dxc(i,j),j=1,3),i=1,3)
|
|
ENDIF
|
|
ENDIF
|
|
5555 FORMAT(1x,f12.5,1x,f12.5,1x,f12.5/ &
|
|
& 1x,f12.5,1x,f12.5,1x,f12.5/ &
|
|
& 1x,f12.5,1x,f12.5,1x,f12.5//)
|
|
!
|
|
RETURN
|
|
END SUBROUTINE vofrho
|
|
|
|
!
|
|
!----------------------------------------------------------------------
|
|
SUBROUTINE checkrho(nnr,nspin,rhor,rmin,rmax,rsum,rnegsum)
|
|
!----------------------------------------------------------------------
|
|
!
|
|
! check \int rho(r)dr and the negative part of rho
|
|
!
|
|
USE kinds, ONLY: DP
|
|
USE mp, ONLY: mp_sum
|
|
USE mp_global, ONLY: intra_image_comm
|
|
|
|
IMPLICIT NONE
|
|
|
|
INTEGER nnr, nspin
|
|
REAL(DP) rhor(nnr,nspin), rmin, rmax, rsum, rnegsum
|
|
!
|
|
REAL(DP) roe
|
|
INTEGER ir, iss
|
|
!
|
|
rsum =0.0
|
|
rnegsum=0.0
|
|
rmin =100.
|
|
rmax =0.0
|
|
DO iss = 1, nspin
|
|
DO ir = 1, nnr
|
|
roe = rhor(ir,iss)
|
|
rsum = rsum + roe
|
|
IF ( roe < 0.0 ) rnegsum = rnegsum + roe
|
|
rmax = MAX( rmax, roe )
|
|
rmin = MIN( rmin, roe )
|
|
END DO
|
|
END DO
|
|
CALL mp_sum( rsum, intra_image_comm )
|
|
CALL mp_sum( rnegsum, intra_image_comm )
|
|
RETURN
|
|
END SUBROUTINE checkrho
|
|
!______________________________________________________________________
|
|
|