mirror of https://gitlab.com/QEF/q-e.git
182 lines
6.3 KiB
Fortran
182 lines
6.3 KiB
Fortran
!
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! Copyright (C) 2001-2018 Quantum ESPRESSO group
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! This file is distributed under the terms of the
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! GNU General Public License. See the file `License'
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! in the root directory of the present distribution,
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! or http://www.gnu.org/copyleft/gpl.txt .
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!
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!----------------------------------------------------------------------------
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SUBROUTINE setup_nscf ( newgrid, xq, elph_mat )
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!----------------------------------------------------------------------------
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!
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! ... This routine initializes variables for the non-scf calculations at k
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! ... and k+q required by the linear response calculation at finite q.
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! ... In particular: finds the symmetry group of the crystal that leaves
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! ... the phonon q-vector (xq) or the single atomic displacement (modenum)
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! ... unchanged; determines the k- and k+q points in the irreducible BZ
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! ... Needed on input (read from data file):
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! ... "nsym" crystal symmetries s, t_rev, "nrot" lattice symetries "s"
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! ... "nkstot" k-points in the irreducible BZ wrt lattice symmetry
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! ... Produced on output:
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! ... symmetries ordered with the "nsymq" phonon symmetries first
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! ... "nkstot" k- and k+q-points in the IBZ calculated for the phonon sym.)
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! ... Misc. data needed for running the non-scf calculation
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!
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USE kinds, ONLY : DP
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USE parameters, ONLY : npk
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USE io_global, ONLY : stdout
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USE constants, ONLY : pi, degspin
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USE cell_base, ONLY : at, bg
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USE ions_base, ONLY : nat, tau, ityp, zv
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USE force_mod, ONLY : force
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USE basis, ONLY : natomwfc
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USE klist, ONLY : xk, wk, nks, degauss, lgauss, &
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ltetra, nkstot, qnorm
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USE lsda_mod, ONLY : lsda, nspin, current_spin, isk
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USE symm_base, ONLY : s, t_rev, nrot, nsym, time_reversal
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USE wvfct, ONLY : nbnd, nbndx
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USE control_flags, ONLY : ethr, isolve, david, max_cg_iter, &
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noinv, use_para_diag
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USE mp_pools, ONLY : kunit
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USE spin_orb, ONLY : domag
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USE noncollin_module, ONLY : noncolin
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USE start_k, ONLY : nks_start, xk_start, wk_start, &
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nk1, nk2, nk3, k1, k2, k3
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USE paw_variables, ONLY : okpaw
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USE uspp_param, ONLY : n_atom_wfc
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USE ktetra, ONLY : tetra, tetra_type, opt_tetra_init
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USE lr_symm_base, ONLY : nsymq, invsymq, minus_q
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USE control_lr, ONLY : lgamma, ethr_nscf
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!
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IMPLICIT NONE
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!
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REAL (DP), INTENT(IN) :: xq(3)
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LOGICAL, INTENT (IN) :: newgrid
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LOGICAL, INTENT (IN) :: elph_mat ! used to be passed through a module.
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!
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REAL (DP), ALLOCATABLE :: rtau (:,:,:)
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LOGICAL :: magnetic_sym, sym(48)
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LOGICAL :: skip_equivalence
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LOGICAL, EXTERNAL :: check_para_diag
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!
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IF ( .NOT. ALLOCATED( force ) ) ALLOCATE( force( 3, nat ) )
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!
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! ... threshold for diagonalization ethr
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!
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ethr = ethr_nscf
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!
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! ... variables for iterative diagonalization
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! ... Davdson: isolve=0, david=4 ; CG: isolve=1, david=1
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isolve = 0
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david = 4
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nbndx = david*nbnd
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max_cg_iter=20
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natomwfc = n_atom_wfc( nat, ityp, noncolin )
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!
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use_para_diag = check_para_diag( nbnd )
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!
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! ... Symmetry and k-point section
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!
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! ... time_reversal = use q=>-q symmetry for k-point generation
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!
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magnetic_sym = noncolin .AND. domag
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!
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! ... smallg_q flags in symmetry operations of the crystal
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! ... that are not symmetry operations of the small group of q
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!
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CALL set_small_group_of_q(nsymq,invsymq,minus_q)
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!
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! ... Input k-points are assumed to be given in the IBZ of the Bravais
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! ... lattice, with the full point symmetry of the lattice.
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!
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if( nks_start > 0 .AND. .NOT. newgrid ) then
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!
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! In this case I keep the same points of the Charge density
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! calculations
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!
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nkstot = nks_start
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xk(:,1:nkstot) = xk_start(:,1:nkstot)
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wk(1:nkstot) = wk_start(1:nkstot)
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else
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!
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! In this case I generate a new set of k-points
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!
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! In the case of electron-phonon matrix element with wannier functions
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! (and possibly in other cases as well) the k-points should not be reduced
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!
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skip_equivalence = elph_mat
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CALL kpoint_grid ( nrot, time_reversal, skip_equivalence, s, t_rev, &
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bg, nk1*nk2*nk3, k1,k2,k3, nk1,nk2,nk3, nkstot, xk, wk)
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endif
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!
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! ... If some symmetries of the lattice are missing in the crystal,
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! ... "irreducible_BZ" computes the missing k-points.
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!
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if(.not.elph_mat) &
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CALL irreducible_BZ (nrot, s, nsymq, minus_q, magnetic_sym, &
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at, bg, npk, nkstot, xk, wk, t_rev)
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!
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! ... add k+q to the list of k
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!
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CALL set_kplusq( xk, wk, xq, nkstot, npk )
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!
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! ... set the granularity for k-point distribution
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!
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IF ( lgamma ) THEN
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kunit = 1
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ELSE
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kunit = 2
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ENDIF
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!
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! ... Map each k point in the irr.-BZ into tetrahedra
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!
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IF ( ltetra .AND. (tetra_type /= 0) ) THEN
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IF (ALLOCATED(tetra)) DEALLOCATE(tetra)
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CALL opt_tetra_init(nsymq, s, time_reversal .AND. minus_q, t_rev, at, bg,&
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npk, k1, k2, k3, nk1, nk2, nk3, nkstot, xk, kunit)
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END IF
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!
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IF ( lsda ) THEN
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!
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! ... LSDA case: two different spin polarizations,
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! ... each with its own kpoints
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!
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if (nspin /= 2) call errore ('setup_nscf','nspin should be 2; check iosys',1)
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!
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CALL set_kup_and_kdw( xk, wk, isk, nkstot, npk )
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!
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ELSE IF ( noncolin ) THEN
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!
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! ... noncolinear magnetism: potential and charge have dimension 4 (1+3)
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!
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if (nspin /= 4) call errore ('setup_nscf','nspin should be 4; check iosys',1)
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current_spin = 1
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!
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ELSE
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!
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! ... LDA case: the two spin polarizations are identical
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!
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wk(1:nkstot) = wk(1:nkstot) * degspin
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current_spin = 1
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!
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IF ( nspin /= 1 ) &
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CALL errore( 'setup_nscf', 'nspin should be 1; check iosys', 1 )
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!
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END IF
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!
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IF ( nkstot > npk ) CALL errore( 'setup_nscf', 'too many k points', nkstot )
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!
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! ...notice: qnorm is used by allocate_nlpot to determine
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! the correct size of the interpolation table "qrad"
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!
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qnorm = sqrt(xq(1)**2 + xq(2)**2 + xq(3)**2)
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!
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! ... distribute k-points (and their weights and spin indices)
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!
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CALL divide_et_impera( nkstot, xk, wk, isk, nks )
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!
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RETURN
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!
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END SUBROUTINE setup_nscf
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