! ! Copyright (C) 2001 PWSCF group ! This file is distributed under the terms of the ! GNU General Public License. See the file `License' ! in the root directory of the present distribution, ! or http://www.gnu.org/copyleft/gpl.txt . ! !---------------------------------------------------------------------- subroutine dvanqq !---------------------------------------------------------------------- ! ! This routine calculates four integrals of the Q functions and ! its derivatives with c V_loc and V_eff which are used ! to compute term dV_bare/dtau * psi in addusdvqpsi and in addusdynmat. ! The result is stored in int1,int2,int4,int5. The routine is called ! only once. int4 and int5 are deallocated after use in ! addusdynmat, and int1 and int2 saved on disk by that routine. ! #include "machine.h" use pwcom use parameters, only : DP use phcom implicit none ! ! And the local variables ! integer :: na, nb, ig, nta, ntb, ir, ih, jh, ijh, ipol, jpol, is ! counter on atoms ! counter on G vectors ! counter on atomic types ! counter on real mesh ! counter on beta functions ! counter on polarizations ! counter on spin real(kind=DP), allocatable :: qmod (:), qmodg (:), qpg (:,:), & ylmkq (:,:), ylmk0 (:,:) ! the modulus of q+G ! the modulus of G ! the q+G vectors ! the spherical harmonics ! the spherical harmonics complex(kind=DP) :: fact, fact1, ZDOTC complex(kind=DP), allocatable :: sk (:), aux1 (:), aux2 (:),& aux3 (:), aux5 (:,:,:), veff (:,:) complex(kind=DP), pointer :: qgmq (:) ! auxiliary variables ! the scalar product function ! auxiliary variable ! a mesh space for d V_loc /dtau ! a mesh space ! a mesh space ! a mesh space ! a mesh space for the FFT of the V_eff ! the augmentation function at q+G if (recover) return if (.not.okvan) return call start_clock ('dvanqq') call setv (2 * nhm * nhm * 3 * nat * nspin, 0.d0, int1, 1) call setv (2 * nhm * nhm * 3 * nat * nat, 0.d0, int2, 1) call setv (nhm * (nhm + 1) * 3 * 3 * nat * nspin, 0.d0, int4, 1) call setv (nhm * (nhm + 1) * 3 * 3 * nat * nat, 0.d0, int5, 1) allocate (sk ( ngm)) allocate (aux1( ngm)) allocate (aux2( ngm)) allocate (aux3( ngm)) allocate (aux5( ngm ,nat, 3 )) allocate (qmodg( ngm)) allocate (veff ( nrxx , nspin)) allocate (ylmk0( ngm , lqx * lqx)) if (.not.lgamma) then allocate (ylmkq(ngm , lqx * lqx)) allocate (qpg (3, ngm)) allocate (qmod( ngm)) allocate (qgmq( ngm)) else qgmq =>qgm endif ! ! compute spherical harmonics ! call ylmr2 (lqx * lqx, ngm, g, gg, ylmk0) do ig = 1, ngm qmodg (ig) = sqrt (gg (ig) ) enddo if (.not.lgamma) then call setqmod (ngm, xq, g, qmod, qpg) call ylmr2 (lqx * lqx, ngm, qpg, qmod, ylmkq) do ig = 1, ngm qmod (ig) = sqrt (qmod (ig) ) enddo endif ! ! we start by computing the FT of the effective potential ! do is = 1, nspin do ir = 1, nrxx veff (ir, is) = DCMPLX (vltot (ir) + vr (ir, is), 0.d0) enddo call cft3 (veff (1, is), nr1, nr2, nr3, nrx1, nrx2, nrx3, - 1) enddo ! ! ! We compute here four of the five integrals needed in the phonon ! fact1 = DCMPLX (0.d0, - tpiba * omega) do na = 1, nat nta = ityp (na) do ig = 1, ngm sk (ig) = vlocq (ig, nta) * eigts1 (ig1 (ig), na) * eigts2 (ig2 ( & ig), na) * eigts3 (ig3 (ig), na) enddo do ipol = 1, 3 do ig = 1, ngm aux5 (ig, na, ipol) = sk (ig) * (g (ipol, ig) + xq (ipol) ) enddo enddo enddo do ntb = 1, ntyp if (tvanp (ntb) ) then ijh = 0 do ih = 1, nh (ntb) do jh = ih, nh (ntb) ijh = ijh + 1 ! ! compute the augmentation function ! call qvan2 (ngm, ih, jh, ntb, qmodg, qgm, ylmk0) if (.not.lgamma) call qvan2 (ngm, ih, jh, ntb, qmod, qgmq, & ylmkq) ! ! NB: for this integral the moving atom and the atom of Q ! do not necessarily coincide ! ! do nb = 1, nat if (ityp (nb) .eq.ntb) then do ig = 1, ngm aux1 (ig) = qgmq (ig) * eigts1 (ig1 (ig), nb) * eigts2 (ig2 & (ig), nb) * eigts3 (ig3 (ig), nb) enddo do na = 1, nat fact = eigqts (na) * conjg (eigqts (nb) ) ! ! nb is the atom of the augmentation function ! do ipol = 1, 3 int2 (ih, jh, ipol, na, nb) = fact * fact1 * ZDOTC (ngm, & aux1, 1, aux5 (1, na, ipol), 1) do jpol = 1, 3 if (jpol.ge.ipol) then do ig = 1, ngm aux3 (ig) = aux5 (ig, na, ipol) * (g (jpol, ig) + xq ( & jpol) ) enddo int5 (ijh, ipol, jpol, na, nb) = conjg (fact) * tpiba2 * & omega * ZDOTC (ngm, aux3, 1, aux1, 1) else int5 (ijh, ipol, jpol, na, nb) = int5 (ijh, jpol, ipol, & na, nb) endif enddo enddo enddo if (.not.lgamma) then do ig = 1, ngm aux1 (ig) = qgm (ig) * eigts1 (ig1 (ig), nb) * eigts2 ( & ig2 (ig), nb) * eigts3 (ig3 (ig), nb) enddo endif do is = 1, nspin do ipol = 1, 3 do ig = 1, ngm aux2 (ig) = veff (nl (ig), is) * g (ipol, ig) enddo int1 (ih, jh, ipol, nb, is) = - fact1 * ZDOTC (ngm, aux1, 1, & aux2, 1) do jpol = 1, 3 if (jpol.ge.ipol) then do ig = 1, ngm aux3 (ig) = aux2 (ig) * g (jpol, ig) enddo int4 (ijh, ipol, jpol, nb, is) = - tpiba2 * omega * & ZDOTC (ngm, aux3, 1, aux1, 1) else int4 (ijh, ipol, jpol, nb, is) = int4 (ijh, jpol, ipol, & nb, is) endif enddo enddo enddo endif enddo enddo enddo do ih = 1, nh (ntb) do jh = ih + 1, nh (ntb) ! ! We use the symmetry properties of the integral factor ! do nb = 1, nat if (ityp (nb) .eq.ntb) then do ipol = 1, 3 do is = 1, nspin int1 (jh, ih, ipol, nb, is) = int1 (ih, jh, ipol, nb, is) enddo do na = 1, nat int2 (jh, ih, ipol, na, nb) = int2 (ih, jh, ipol, na, nb) enddo enddo endif enddo enddo enddo endif enddo #ifdef PARA call reduce (2 * nhm * nhm * 3 * nat * nspin, int1) call reduce (2 * nhm * nhm * 3 * nat * nat, int2) call reduce (nhm * (nhm + 1) * 3 * 3 * nat * nspin, int4) call reduce (nhm * (nhm + 1) * 3 * 3 * nat * nat, int5) #endif ! do ih=1,nh(1) ! do jh=1,nh(1) ! do ipol=1,3 ! write(6,'(3i5,2f20.10)') ipol,ih,jh,int2(ih,jh,ipol,1,1) ! enddo ! enddo ! enddo ! call stop_ph(.true.) if (.not.lgamma) then deallocate(qgmq) deallocate (qmod) deallocate (qpg) deallocate (ylmkq) endif deallocate (ylmk0) deallocate (veff) deallocate (qmodg) deallocate (aux5) deallocate (aux3) deallocate (aux2) deallocate (aux1) deallocate (sk) call stop_clock ('dvanqq') return end subroutine dvanqq