modxcifc.f90

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! Copyright (C) 2002-2005 J. K. Dewhurst, S. Sharma and C. Ambrosch-Draxl.
! This file is distributed under the terms of the GNU General Public License.
! See the file COPYING for license details.

module modxcifc

use libxcifc

contains

!BOP
! !ROUTINE: xcifc
! !INTERFACE:
subroutine xcifc(xctype,n,c_tb09,tempa,rho,rhoup,rhodn,grho,gup,gdn,g2rho,g2up,&
 g2dn,g3rho,g3up,g3dn,grho2,gup2,gdn2,gupdn,tau,tauup,taudn,ex,ec,vx,vc,vxup, &
 vxdn,vcup,vcdn,dxdgr2,dxdgu2,dxdgd2,dxdgud,dcdgr2,dcdgu2,dcdgd2,dcdgud,dxdg2r,&
 dxdg2u,dxdg2d,dcdg2r,dcdg2u,dcdg2d,wx,wxup,wxdn,wc,wcup,wcdn,dtdr,dtdru,dtdrd,&
 dtdgr2,dtdgu2,dtdgd2,dtdg2r,dtdg2u,dtdg2d)
! !INPUT/OUTPUT PARAMETERS:
!   xctype : type of exchange-correlation functional (in,integer(3))
!   n      : number of density points (in,integer)
!   c_tb09 : Tran-Blaha '09 constant c (in,real,optional)
!   tempa  : temperature in atomic units (in,real,optional)
!   rho    : spin-unpolarised charge density (in,real(n),optional)
!   rhoup  : spin-up charge density (in,real(n),optional)
!   rhodn  : spin-down charge density (in,real(n),optional)
!   grho   : |grad rho| (in,real(n),optional)
!   gup    : |grad rhoup| (in,real(n),optional)
!   gdn    : |grad rhodn| (in,real(n),optional)
!   g2rho  : grad^2 rho (in,real(n),optional)
!   g2up   : grad^2 rhoup (in,real(n),optional)
!   g2dn   : grad^2 rhodn (in,real(n),optional)
!   g3rho  : (grad rho).(grad |grad rho|) (in,real(n),optional)
!   g3up   : (grad rhoup).(grad |grad rhoup|) (in,real(n),optional)
!   g3dn   : (grad rhodn).(grad |grad rhodn|) (in,real(n),optional)
!   grho2  : |grad rho|^2 (in,real(n),optional)
!   gup2   : |grad rhoup|^2 (in,real(n),optional)
!   gdn2   : |grad rhodn|^2 (in,real(n),optional)
!   gupdn  : (grad rhoup).(grad rhodn) (in,real(n),optional)
!   tau    : kinetic energy density (in,real(n),optional)
!   tauup  : spin-up kinetic energy density (in,real(n),optional)
!   taudn  : spin-down kinetic energy density (in,real(n),optional)
!   ex     : exchange energy density (out,real(n),optional)
!   ec     : correlation energy density (out,real(n),optional)
!   vx     : spin-unpolarised exchange potential (out,real(n),optional)
!   vc     : spin-unpolarised correlation potential (out,real(n),optional)
!   vxup   : spin-up exchange potential (out,real(n),optional)
!   vxdn   : spin-down exchange potential (out,real(n),optional)
!   vcup   : spin-up correlation potential (out,real(n),optional)
!   vcdn   : spin-down correlation potential (out,real(n),optional)
!   dxdgr2 : de_x/d(|grad rho|^2) (out,real(n),optional)
!   dxdgu2 : de_x/d(|grad rhoup|^2) (out,real(n),optional)
!   dxdgd2 : de_x/d(|grad rhodn|^2) (out,real(n),optional)
!   dxdgud : de_x/d((grad rhoup).(grad rhodn)) (out,real(n),optional)
!   dcdgr2 : de_c/d(|grad rho|^2) (out,real(n),optional)
!   dcdgu2 : de_c/d(|grad rhoup|^2) (out,real(n),optional)
!   dcdgd2 : de_c/d(|grad rhodn|^2) (out,real(n),optional)
!   dcdgud : de_c/d((grad rhoup).(grad rhodn)) (out,real(n),optional)
!   dxdg2r : de_x/d(grad^2 rho) (out,real(n),optional)
!   dxdg2u : de_x/d(grad^2 rhoup) (out,real(n),optional)
!   dxdg2d : de_x/d(grad^2 rhodn) (out,real(n),optional)
!   dcdg2r : de_c/d(grad^2 rho) (out,real(n),optional)
!   dcdg2u : de_c/d(grad^2 rhoup) (out,real(n),optional)
!   dcdg2d : de_c/d(grad^2 rhodn) (out,real(n),optional)
!   wx     : de_x/dtau (out,real(n),optional)
!   wxup   : de_x/dtauup (out,real(n),optional)
!   wxdn   : de_x/dtaudn (out,real(n),optional)
!   wc     : de_c/dtau (out,real(n),optional)
!   wcup   : de_c/dtauup (out,real(n),optional)
!   wcdn   : de_c/dtaudn (out,real(n),optional)
!   dtdr   : dtau/drho (out,real(n),optional)
!   dtdru  : dtauup/drhoup (out,real(n),optional)
!   dtdrd  : dtaudn/drhodn (out,real(n),optional)
!   dtdgr2 : dtau/d|grad rho|^2 (out,real(n),optional)
!   dtdgu2 : dtauup/d(|grad rhoup|^2) (out,real(n),optional)
!   dtdgd2 : dtaudn/d(|grad rhodn|^2) (out,real(n),optional)
!   dtdg2r : dtau/d(grad^2 rho) (out,real(n),optional)
!   dtdg2u : dtauup/d(grad^2 rhoup) (out,real(n),optional)
!   dtdg2d : dtaudn/d(grad^2 rhodn) (out,real(n),optional)
! !DESCRIPTION:
!   Interface to the exchange-correlation routines. In the most general case
!   (meta-GGA), the exchange-correlation energy is given by
!   $$ E_{xc}[\rho^{\uparrow},\rho^{\downarrow}]=\int d^3r\,
!    \rho({\bf r})\,\varepsilon_{xc}(\rho^{\uparrow},\rho^{\downarrow},
!    |\nabla\rho|,|\nabla\rho^{\uparrow}|,|\nabla\rho^{\downarrow}|,
!    \nabla^2\rho^{\uparrow},\nabla^2\rho^{\downarrow},\tau), $$
!   where $\rho({\bf r})=\rho^{\uparrow}({\bf r})+\rho^{\downarrow}({\bf r})$ is
!   the density;
!   $$ \tau({\bf r})\equiv\sum_{i\;{\rm occ}}\nabla\psi({\bf r})\cdot
!   \nabla\psi({\bf r}) $$
!   is twice the spin-contracted kinetic energy density; and $\varepsilon_{xc}$
!   is the exchange-correlation energy per electron.
!
! !REVISION HISTORY:
!   Created October 2002 (JKD)
!EOP
!BOC
implicit none
! mandatory arguments
integer, intent(in) :: xctype(3),n
! optional arguments
real(8), optional, intent(in) :: c_tb09,tempa
real(8), optional, intent(in) :: rho(n),rhoup(n),rhodn(n)
real(8), optional, intent(in) :: grho(n),gup(n),gdn(n)
real(8), optional, intent(in) :: g2rho(n),g2up(n),g2dn(n)
real(8), optional, intent(in) :: g3rho(n),g3up(n),g3dn(n)
real(8), optional, intent(in) :: grho2(n),gup2(n),gdn2(n),gupdn(n)
real(8), optional, intent(in) :: tau(n),tauup(n),taudn(n)
real(8), optional, intent(out) :: ex(n),ec(n),vx(n),vc(n)
real(8), optional, intent(out) :: vxup(n),vxdn(n),vcup(n),vcdn(n)
real(8), optional, intent(out) :: dxdgr2(n),dxdgu2(n),dxdgd2(n),dxdgud(n)
real(8), optional, intent(out) :: dxdg2r(n),dxdg2u(n),dxdg2d(n)
real(8), optional, intent(out) :: wx(n),wxup(n),wxdn(n)
real(8), optional, intent(out) :: dcdgr2(n),dcdgu2(n),dcdgd2(n),dcdgud(n)
real(8), optional, intent(out) :: dcdg2r(n),dcdg2u(n),dcdg2d(n)
real(8), optional, intent(out) :: wc(n),wcup(n),wcdn(n)
real(8), optional, intent(out) :: dtdr(n),dtdru(n),dtdrd(n)
real(8), optional, intent(out) :: dtdgr2(n),dtdgu2(n),dtdgd2(n)
real(8), optional, intent(out) :: dtdg2r(n),dtdg2u(n),dtdg2d(n)
! local variables
real(8) kappa,mu,beta
! allocatable arrays
real(8), allocatable :: ra(:,:)
if (n < 1) then
  write(*,*)
  write(*,'("Error(xcifc): n < 1 : ",I8)') n
  write(*,*)
  stop
end if
select case(abs(xctype(1)))
case(1)
! No density-derived exchange-correlation energy or potential
  if (present(ex)) ex(1:n)=0.d0
  if (present(ec)) ec(1:n)=0.d0
  if (present(vx)) vx(1:n)=0.d0
  if (present(vc)) vc(1:n)=0.d0
  if (present(vxup)) vxup(1:n)=0.d0
  if (present(vxdn)) vxdn(1:n)=0.d0
  if (present(vcup)) vcup(1:n)=0.d0
  if (present(vcdn)) vcdn(1:n)=0.d0
case(2)
! Perdew-Zunger parameterisation of Ceperley-Alder electron gas
! J. Perdew and A. Zunger, Phys. Rev. B 23, 5048 (1981)
! D. M. Ceperly and B. J. Alder, Phys. Rev. Lett. 45, 566 (1980)
  if (present(rho).and.present(ex).and.present(ec).and.present(vx) &
   .and.present(vc)) then
    call xc_pzca(n,rho,ex,ec,vx,vc)
  else
    goto 10
  end if
case(3)
! Perdew-Wang parameterisation of the spin-polarised Ceperley-Alder electron gas
! J. Perdew and Y. Wang, Phys. Rev. B 45, 13244 (1992)
! D. M. Ceperly and B. J. Alder, Phys. Rev. Lett. 45, 566 (1980)
  if (present(rhoup).and.present(rhodn).and.present(ex).and.present(ec) &
   .and.present(vxup).and.present(vxdn).and.present(vcup) &
   .and.present(vcdn)) then
! spin-polarised density
    call xc_pwca(n,rhoup,rhodn,ex,ec,vxup,vxdn,vcup,vcdn)
  else if (present(rho).and.present(ex).and.present(ec).and.present(vx) &
   .and.present(vc)) then
! divide spin-unpolarised density into up and down
    allocate(ra(n,2))
    ra(1:n,1)=0.5d0*rho(1:n)
    call xc_pwca(n,ra,ra,ex,ec,vx,ra(:,2),vc,ra(:,2))
    deallocate(ra)
  else
    goto 10
  end if
case(4)
! X-alpha approximation
! J. C. Slater, Phys. Rev. 81, 385 (1951)
  if (present(rho).and.present(ex).and.present(ec).and.present(vx) &
   .and.present(vc)) then
    call xc_xalpha(n,rho,ex,vx)
! set correlation energy and potential to zero
    ec(1:n)=0.d0
    vc(1:n)=0.d0
  else
    goto 10
  end if
case(5)
! U. von Barth and L. Hedin parameterisation of LSDA
! J. Phys. C, 5, 1629 (1972)
  if (present(rhoup).and.present(rhodn).and.present(ex).and.present(ec) &
   .and.present(vxup).and.present(vxdn).and.present(vcup) &
   .and.present(vcdn)) then
! spin-polarised density
    call xc_vbh(n,rhoup,rhodn,ex,ec,vxup,vxdn,vcup,vcdn)
  else if (present(rho).and.present(ex).and.present(ec).and.present(vx) &
   .and.present(vc)) then
! divide spin-unpolarised density into up and down
    allocate(ra(n,2))
    ra(1:n,1)=0.5d0*rho(1:n)
    call xc_vbh(n,ra,ra,ex,ec,vx,ra(:,2),vc,ra(:,2))
    deallocate(ra)
  else
    goto 10
  end if
case(20,21,22)
! original PBE kappa
  kappa=0.804d0
  if (xctype(1) == 21) then
! Zhang-Yang kappa
    kappa=1.245d0
  end if
! original PBE mu and beta
  mu=0.2195149727645171d0
  beta=0.06672455060314922d0
  if (xctype(1) == 22) then
! PBEsol parameters
    mu=10.d0/81.d0
    beta=0.046d0
  end if
! Perdew-Burke-Ernzerhof generalised gradient approximation
! Phys. Rev. Lett. 77, 3865 (1996); 78, 1396(E) (1997)
! Revised PBE, Zhang-Yang, Phys. Rev. Lett. 80, 890 (1998)
  if (present(rhoup).and.present(rhodn).and.present(grho).and.present(gup) &
   .and.present(gdn).and.present(g2up).and.present(g2dn).and.present(g3rho) &
   .and.present(g3up).and.present(g3dn).and.present(ex).and.present(ec) &
   .and.present(vxup).and.present(vxdn).and.present(vcup) &
   .and.present(vcdn)) then
    call xc_pbe(n,kappa,mu,beta,rhoup,rhodn,grho,gup,gdn,g2up,g2dn,g3rho,g3up, &
     g3dn,ex,ec,vxup,vxdn,vcup,vcdn)
  else if (present(rho).and.present(grho).and.present(g2rho) &
   .and.present(g3rho).and.present(ex).and.present(ec).and.present(vx) &
   .and.present(vc)) then
    allocate(ra(n,5))
    ra(1:n,1)=0.5d0*rho(1:n)
    ra(1:n,2)=0.5d0*grho(1:n)
    ra(1:n,3)=0.5d0*g2rho(1:n)
    ra(1:n,4)=0.25d0*g3rho(1:n)
    call xc_pbe(n,kappa,mu,beta,ra,ra,grho,ra(:,2),ra(:,2),ra(:,3),ra(:,3), &
     g3rho,ra(:,4),ra(:,4),ex,ec,vx,ra(:,5),vc,ra(:,5))
    deallocate(ra)
  else
    goto 10
  end if
case(26)
! Wu-Cohen exchange with PBE correlation generalised gradient functional
! Zhigang Wu and R. E. Cohen, Phys. Rev. B 73, 235116 (2006)
  if (present(rho).and.present(grho).and.present(g2rho).and.present(g3rho) &
   .and.present(ex).and.present(ec).and.present(vx).and.present(vc)) then
    call xc_wc06(n,rho,grho,g2rho,g3rho,ex,ec,vx,vc)
  else
    goto 10
  end if
case(30)
! Armiento-Mattsson generalised gradient functional
! R. Armiento and A. E. Mattsson, Phys. Rev. B 72, 085108 (2005)
  if (present(rho).and.present(grho).and.present(g2rho).and.present(g3rho) &
   .and.present(ex).and.present(ec).and.present(vx).and.present(vc)) then
    call xc_am05(n,rho,grho,g2rho,g3rho,ex,ec,vx,vc)
  else
    goto 10
  end if
case(50)
! Thomas-Fermi kinetic energy functional derivative δτ(r')/δρ(r)
  if (present(rhoup).and.present(rhodn).and.present(dtdru) &
   .and.present(dtdrd)) then
    call k_tf_sp(n,rhoup,rhodn,dtdru,dtdrd)
    if (present(dtdgu2)) dtdgu2(1:n)=0.d0
    if (present(dtdgd2)) dtdgd2(1:n)=0.d0
  else if (present(rho).and.present(dtdr)) then
    call k_tf(n,rho,dtdr)
    if (present(dtdgr2)) dtdgr2(1:n)=0.d0
  else
    goto 10
  end if
case(51)
! Thomas-Fermi kinetic energy functional derivative scaled by the ratio of the
! exact τ to the TF τ
  if (present(rhoup).and.present(rhodn).and.present(tauup).and.present(taudn) &
   .and.present(dtdru).and.present(dtdrd)) then
    call k_tfsc_sp(n,rhoup,rhodn,tauup,taudn,dtdru,dtdrd)
    if (present(dtdgu2)) dtdgu2(1:n)=0.d0
    if (present(dtdgd2)) dtdgd2(1:n)=0.d0
  else if (present(rho).and.present(tau).and.present(dtdr)) then
    call k_tfsc(n,rho,tau,dtdr)
    if (present(dtdgr2)) dtdgr2(1:n)=0.d0
  else
    goto 10
  end if
case(52)
! Thomas-Fermi-von Weizsacker kinetic energy functional derivative
  if (present(rhoup).and.present(rhodn).and.present(gup2).and.present(gdn2) &
   .and.present(dtdru).and.present(dtdrd).and.present(dtdgu2) &
   .and.present(dtdgd2)) then
    call k_tfvw_sp(n,rhoup,rhodn,gup2,gdn2,dtdru,dtdrd,dtdgu2,dtdgd2)
  else if (present(rho).and.present(grho2).and.present(dtdr) &
   .and.present(dtdgr2)) then
    call k_tfvw(n,rho,grho2,dtdr,dtdgr2)
  else
    goto 10
  end if
case(100)
! libxc library functionals
  if (present(rhoup).and.present(rhodn).and.present(g2up).and.present(g2dn) &
   .and.present(gup2).and.present(gdn2).and.present(gupdn).and.present(tauup) &
   .and.present(taudn).and.present(vxup).and.present(vxdn).and.present(vcup) &
   .and.present(vcdn).and.present(dxdgu2).and.present(dxdgd2) &
   .and.present(dxdgud).and.present(dcdgu2).and.present(dcdgd2) &
   .and.present(dcdgud).and.present(dxdg2u).and.present(dxdg2d) &
   .and.present(dcdg2u).and.present(dcdg2d).and.present(wxup).and.present(wxdn)&
   .and.present(wcup).and.present(wcdn)) then
! spin-polarised meta-GGA
    if (present(ex).and.present(ec)) then
! energy functional
      call xcifc_libxc(xctype,n,rhoup=rhoup,rhodn=rhodn,g2up=g2up,g2dn=g2dn, &
       gup2=gup2,gdn2=gdn2,gupdn=gupdn,tauup=tauup,taudn=taudn,ex=ex,ec=ec, &
       vxup=vxup,vxdn=vxdn,vcup=vcup,vcdn=vcdn,dxdgu2=dxdgu2,dxdgd2=dxdgd2, &
       dxdgud=dxdgud,dcdgu2=dcdgu2,dcdgd2=dcdgd2,dcdgud=dcdgud,dxdg2u=dxdg2u, &
       dxdg2d=dxdg2d,dcdg2u=dcdg2u,dcdg2d=dcdg2d,wxup=wxup,wxdn=wxdn,wcup=wcup,&
       wcdn=wcdn)
    else
! potential-only functional
      call xcifc_libxc(xctype,n,c_tb09=c_tb09,rhoup=rhoup,rhodn=rhodn, &
       g2up=g2up,g2dn=g2dn,gup2=gup2,gdn2=gdn2,gupdn=gupdn,tauup=tauup, &
       taudn=taudn,vxup=vxup,vxdn=vxdn,vcup=vcup,vcdn=vcdn,dxdgu2=dxdgu2, &
       dxdgd2=dxdgd2,dxdgud=dxdgud,dcdgu2=dcdgu2,dcdgd2=dcdgd2,dcdgud=dcdgud, &
       dxdg2u=dxdg2u,dxdg2d=dxdg2d,dcdg2u=dcdg2u,dcdg2d=dcdg2d,wxup=wxup, &
       wxdn=wxdn,wcup=wcup,wcdn=wcdn)
    end if
  else if (present(rhoup).and.present(rhodn).and.present(gup2) &
   .and.present(gdn2).and.present(gupdn).and.present(ex).and.present(ec) &
   .and.present(vxup).and.present(vxdn).and.present(vcup).and.present(vcdn) &
   .and.present(dxdgu2).and.present(dxdgd2).and.present(dxdgud) &
   .and.present(dcdgu2).and.present(dcdgd2).and.present(dcdgud)) then
! spin-polarised GGA
    call xcifc_libxc(xctype,n,rhoup=rhoup,rhodn=rhodn,gup2=gup2,gdn2=gdn2, &
     gupdn=gupdn,ex=ex,ec=ec,vxup=vxup,vxdn=vxdn,vcup=vcup,vcdn=vcdn, &
     dxdgu2=dxdgu2,dxdgd2=dxdgd2,dxdgud=dxdgud,dcdgu2=dcdgu2,dcdgd2=dcdgd2, &
     dcdgud=dcdgud)
  else if (present(rhoup).and.present(rhodn).and.present(g2up) &
   .and.present(g2dn).and.present(gup2).and.present(gdn2).and.present(tauup) &
   .and.present(taudn).and.present(dtdru).and.present(dtdrd) &
   .and.present(dtdg2u).and.present(dtdg2d).and.present(dtdgu2) &
   .and.present(dtdgd2).and.present(wxup).and.present(wxdn)) then
! spin-polarised kinetic energy functional
    call xcifc_libxc(xctype,n,rhoup=rhoup,rhodn=rhodn,g2up=g2up,g2dn=g2dn, &
     gup2=gup2,gdn2=gdn2,tauup=tauup,taudn=taudn,vxup=dtdru,vxdn=dtdrd, &
     dxdg2u=dtdg2u,dxdg2d=dtdg2d,dxdgu2=dtdgu2,dxdgd2=dtdgd2,wxup=wxup, &
     wxdn=wxdn)
  else if (present(rhoup).and.present(rhodn).and.present(ex).and.present(ec) &
   .and.present(vxup).and.present(vxdn).and.present(vcup) &
   .and.present(vcdn)) then
! spin-polarised LSDA
    call xcifc_libxc(xctype,n,tempa=tempa,rhoup=rhoup,rhodn=rhodn,ex=ex,ec=ec, &
     vxup=vxup,vxdn=vxdn,vcup=vcup,vcdn=vcdn)
  else if (present(rho).and.present(g2rho).and.present(grho2).and.present(tau) &
   .and.present(vx).and.present(vc).and.present(dxdgr2).and.present(dcdgr2) &
   .and.present(dxdg2r).and.present(dcdg2r).and.present(wx).and.present(wc))then
! spin-unpolarised meta-GGA
    if (present(ex).and.present(ec)) then
! energy functional
      call xcifc_libxc(xctype,n,rho=rho,g2rho=g2rho,grho2=grho2,tau=tau,ex=ex, &
       ec=ec,vx=vx,vc=vc,dxdgr2=dxdgr2,dcdgr2=dcdgr2,dxdg2r=dxdg2r, &
       dcdg2r=dcdg2r,wx=wx,wc=wc)
    else
! potential-only functional
      call xcifc_libxc(xctype,n,c_tb09=c_tb09,rho=rho,g2rho=g2rho,grho2=grho2, &
       tau=tau,vx=vx,vc=vc,dxdgr2=dxdgr2,dcdgr2=dcdgr2,dxdg2r=dxdg2r, &
       dcdg2r=dcdg2r,wx=wx,wc=wc)
    end if
  else if (present(rho).and.present(grho2).and.present(ex).and.present(ec) &
   .and.present(vx).and.present(vc).and.present(dxdgr2) &
   .and.present(dcdgr2)) then
! spin-unpolarised GGA
    call xcifc_libxc(xctype,n,rho=rho,grho2=grho2,ex=ex,ec=ec,vx=vx,vc=vc, &
     dxdgr2=dxdgr2,dcdgr2=dcdgr2)
  else if (present(rho).and.present(g2rho).and.present(grho2).and.present(tau) &
   .and.present(dtdr).and.present(dtdgr2).and.present(dtdg2r) &
   .and.present(wx)) then
! spin-unpolarised kinetic energy functional
    call xcifc_libxc(xctype,n,rho=rho,g2rho=g2rho,grho2=grho2,tau=tau,vx=dtdr, &
     dxdgr2=dtdgr2,dxdg2r=dtdg2r,wx=wx)
  else if (present(rho).and.present(ex).and.present(ec).and.present(vx) &
   .and.present(vc)) then
! spin-unpolarised LDA
    call xcifc_libxc(xctype,n,tempa=tempa,rho=rho,ex=ex,ec=ec,vx=vx,vc=vc)
  else
    goto 10
  end if
case default
  write(*,*)
  write(*,'("Error(xcifc): xctype not defined : ",I8)') xctype(1)
  write(*,*)
  stop
end select
! set exchange potential to zero for EXX
if (xctype(1) <= -2) then
  if (present(vx)) vx(1:n)=0.d0
  if (present(vxup)) vxup(1:n)=0.d0
  if (present(vxdn)) vxdn(1:n)=0.d0
end if
return
10 continue
write(*,*)
write(*,'("Error(xcifc): missing arguments for exchange-correlation type ",&
 &3I6)') xctype(:)
write(*,*)
stop
end subroutine
!EOC

!BOP
! !ROUTINE: getxcdata
! !INTERFACE:
subroutine getxcdata(xctype,xcdescr,xcspin,xcgrad,hybrid,hybridc)
! !INPUT/OUTPUT PARAMETERS:
!   xctype  : type of exchange-correlation functional (in,integer(3))
!   xcdescr : description of functional (out,character(264))
!   xcspin  : spin treatment (out,integer)
!   xcgrad  : gradient treatment (out,integer)
!   hybrid  : .true. if functional a hybrid (out,logical)
!   hybridc : hybrid exact exchange mixing coefficient (out,real(8))
! !DESCRIPTION:
!   Returns data on the exchange-correlation functional labeled by {\tt xctype}.
!   The character array {\tt xcdescr} contains a short description of the
!   functional including journal references. The variable {\tt xcspin} is set to
!   1 or 0 for spin-polarised or -unpolarised functionals, respectively. For
!   functionals which require the gradients of the density {\tt xcgrad} is set
!   to 1, otherwise it is set to 0.
!
! !REVISION HISTORY:
!   Created October 2002 (JKD)
!EOP
!BOC
implicit none
! arguments
integer, intent(in) :: xctype(3)
character(264), intent(out) :: xcdescr
integer, intent(out) :: xcspin,xcgrad
logical, intent(out) :: hybrid
real(8), intent(out) :: hybridc
select case(abs(xctype(1)))
case(1)
  xcdescr='No density-derived exchange-correlation energy or potential'
! spin-polarisation or gradient status not required
  xcspin=-1
  xcgrad=-1
case(2)
  xcdescr='Perdew-Zunger/Ceperley-Alder, Phys. Rev. B 23, 5048 (1981)'
  xcspin=0
  xcgrad=0
case(3)
  xcdescr='Perdew-Wang/Ceperley-Alder, Phys. Rev. B 45, 13244 (1992)'
  xcspin=1
  xcgrad=0
case(4)
  xcdescr='X-alpha approximation, J. C. Slater, Phys. Rev. 81, 385 (1951)'
  xcspin=0
  xcgrad=0
case(5)
  xcdescr='von Barth-Hedin, J. Phys. C 5, 1629 (1972)'
  xcspin=1
  xcgrad=0
case(20)
  xcdescr='Perdew-Burke-Ernzerhof, Phys. Rev. Lett. 77, 3865 (1996)'
  xcspin=1
  xcgrad=1
case(21)
  xcdescr='Revised PBE, Zhang-Yang, Phys. Rev. Lett. 80, 890 (1998)'
  xcspin=1
  xcgrad=1
case(22)
  xcdescr='PBEsol, Phys. Rev. Lett. 100, 136406 (2008)'
  xcspin=1
  xcgrad=1
case(26)
  xcdescr='Wu-Cohen exchange + PBE correlation, Phys. Rev. B 73, 235116 (2006)'
  xcspin=0
  xcgrad=1
case(30)
  xcdescr='Armiento-Mattsson functional, Phys. Rev. B 72, 85108 (2005)'
  xcspin=0
  xcgrad=1
case(50)
  xcdescr='Thomas-Fermi kinetic energy functional'
  xcspin=-1
  xcgrad=0
case(51)
  xcdescr='Thomas-Fermi kinetic energy functional scaled by the ratio of the &
   &exact τ to the TF τ'
  xcspin=-1
  xcgrad=0
case(52)
  xcdescr='Thomas-Fermi-von Weizsacker kinetic energy functional'
  xcspin=-1
  xcgrad=1
case(100)
! libxc library functionals
  call xcdata_libxc(xctype,xcdescr,xcspin,xcgrad,hybrid,hybridc)
case default
  write(*,*)
  write(*,'("Error(getxcdata): xctype not defined : ",I8)') xctype(1)
  write(*,*)
  stop
end select
end subroutine
!EOC

end module