mirror of
https://github.com/triqs/dft_tools
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290 lines
12 KiB
FortranFixed
290 lines
12 KiB
FortranFixed
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c ******************************************************************************
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c
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c TRIQS: a Toolbox for Research in Interacting Quantum Systems
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c
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c Copyright (C) 2011 by L. Pourovskii, V. Vildosola, C. Martins, M. Aichhorn
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c
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c TRIQS is free software: you can redistribute it and/or modify it under the
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c terms of the GNU General Public License as published by the Free Software
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c Foundation, either version 3 of the License, or (at your option) any later
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c version.
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c
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c TRIQS is distributed in the hope that it will be useful, but WITHOUT ANY
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c WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS
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c FOR A PARTICULAR PURPOSE. See the GNU General Public License for more
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c details.
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c
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c You should have received a copy of the GNU General Public License along with
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c TRIQS. If not, see <http://www.gnu.org/licenses/>.
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c
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c *****************************************************************************/
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SUBROUTINE timeinv_op(mat,lm,l,isrt)
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C %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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C %% %%
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C %% This subroutine applies the time reversal operation to the %%
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C %% matrix mat which is associated to the l orbital of the atomic %%
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C %% isrt. (matrix size = lm) The matrix mat is assumed to already %%
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C %% be in the desired basis associated to isrt. %%
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C %% The calculation done is : %%
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C %% reptrans*T*conjg((inv(reptrans))*conjg(mat) %%
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C %% %%
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C %% If isrt=0, the matrix mat is assumed to be in the spherical %%
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C %% harmonics basis and no spin is considered. (lm = 2*l+1) %%
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C %% The calculation done is then : T*conjg(mat) %%
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C %% %%
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C %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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C Definiton of the variables :
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C ----------------------------
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USE common_data
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USE reps
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IMPLICIT NONE
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INTEGER :: lm,l,isrt
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COMPLEX(KIND=8), DIMENSION(1:lm,1:lm) :: mat
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COMPLEX(KIND=8), DIMENSION(:,:), ALLOCATABLE :: tinv
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COMPLEX(KIND=8), DIMENSION(:,:), ALLOCATABLE :: tmp_tinv
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COMPLEX(KIND=8), DIMENSION(-l:l,-l:l) :: tmat
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INTEGER :: m,n
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C
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C Definition of the complex conjugation operator in the spherical harmonic basis :
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C --------------------------------------------------------------------------------
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C
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tmat = CMPLX(0.d0,0.d0)
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DO m=-l,l
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tmat(m,-m)=(-1)**m
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END DO
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C
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C
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C Calculation of the Time-reversal operator in the desired representation basis :
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C -------------------------------------------------------------------------------
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C
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IF (isrt==0) THEN
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C The case isrt=0 is a "default case" :
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C mat is in the spherical harmonic basis (without spinor representation)
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ALLOCATE(tinv(1:2*l+1,1:2*l+1))
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tinv(1:2*l+1,1:2*l+1)=tmat(-l:l,-l:l)
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ELSE
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C If the basis representation needs a complete spinor rotation approach (matrices of size 2*(2*l+1) )
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IF (reptrans(l,isrt)%ifmixing) THEN
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ALLOCATE(tinv(1:2*(2*l+1),1:2*(2*l+1)))
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ALLOCATE(tmp_tinv(1:2*(2*l+1),1:2*(2*l+1)))
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tinv = CMPLX(0.d0,0.d0)
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tmp_tinv = CMPLX(0.d0,0.d0)
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C Definition of the time-reversal operator as a spinor-operator (multiplication by -i.sigma_y)
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tinv(1:2*l+1,2*l+2:2*(2*l+1))=-tmat(-l:l,-l:l)
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tinv(2*l+2:2*(2*l+1),1:2*l+1)=tmat(-l:l,-l:l)
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C The time reversal operator is put in the desired basis.
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tmp_tinv(1:2*(2*l+1),1:2*(2*l+1))=MATMUL(
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& reptrans(l,isrt)%transmat(1:2*(2*l+1),1:2*(2*l+1)),
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& tinv(1:2*(2*l+1),1:2*(2*l+1)))
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tinv(1:2*(2*l+1),1:2*(2*l+1))=MATMUL(
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& tmp_tinv(1:2*(2*l+1),1:2*(2*l+1)),
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& TRANSPOSE(reptrans(l,isrt)%transmat
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& (1:2*(2*l+1),1:2*(2*l+1)) ) )
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C the result tinv = (reptrans)*tinv*transpose(reptrans)
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C or tinv_{new_i} = <new_i|lm> tinv_{lm} (<lm|new_i>)*
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C which is exactly the expression of the spinor operator in the new basis.
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DEALLOCATE(tmp_tinv)
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C If the basis representation can be reduce to the up/up block (matrices of size (2*l+1) only)
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ELSE
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ALLOCATE(tinv(1:2*l+1,1:2*l+1))
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ALLOCATE(tmp_tinv(-l:l,-l:l))
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tinv = CMPLX(0.d0,0.d0)
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tmp_tinv = CMPLX(0.d0,0.d0)
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C The time reversal operator is put in the desired basis.
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tmp_tinv(-l:l,-l:l)=MATMUL(
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& reptrans(l,isrt)%transmat(-l:l,-l:l),
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& tmat(-l:l,-l:l) )
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tinv(1:2*l+1,1:2*l+1)=MATMUL(
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& tmp_tinv(-l:l,-l:l),TRANSPOSE(
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& reptrans(l,isrt)%transmat(-l:l,-l:l)) )
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DEALLOCATE(tmp_tinv)
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END IF
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C the result tinv = (reptrans)*tinv*transpose(reptrans)
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C or tinv_{new_i} = <new_i|lm> tinv_{lm} (<lm|new_i>)*
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C which is exactly the expression of the operator in the new basis.
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END IF
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C
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C
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C Multiplication of the matrix mat by the time reversal operator :
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C ----------------------------------------------------------------
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C
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mat(1:lm,1:lm) = MATMUL(
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& tinv(1:lm,1:lm),CONJG(mat(1:lm,1:lm)) )
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DEALLOCATE(tinv)
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C The multiplication is the product of tinv and (mat)*
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C
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RETURN
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END
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SUBROUTINE add_timeinv(Dmat,orbit,norbit)
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C %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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C %% %%
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C %% This subroutine calculates for each density matrix in Dmat %%
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C %% its image by the time-reversal operator and adds it to the %%
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C %% former one to get a time-symmetrized result. %%
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C %% %%
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C %% This operation is done only if the computation is paramagnetic %%
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C %% %%
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C %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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C Definiton of the variables :
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C ----------------------------
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USE common_data
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USE projections
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USE symm
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USE reps
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IMPLICIT NONE
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INTEGER :: norbit
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TYPE(matrix), DIMENSION(nsp,norbit) :: Dmat
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COMPLEX(KIND=8),DIMENSION(:,:,:), ALLOCATABLE :: rot_dmat
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COMPLEX(KIND=8),DIMENSION(:,:), ALLOCATABLE :: time_op
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COMPLEX(KIND=8),DIMENSION(:,:,:), ALLOCATABLE :: tmp_mat
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COMPLEX(KIND=8):: ephase
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TYPE(orbital), DIMENSION(norbit) :: orbit
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INTEGER :: isym, iorb, iatom, jorb, is, is1, l, i
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INTEGER :: isrt, jatom, imult, m
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C
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C
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DO iorb=1,norbit
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l=orbit(iorb)%l
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isrt=orbit(iorb)%sort
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iatom=orbit(iorb)%atom
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C -----------------------------------------------------------------------------------
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C The s-orbitals are a particular case of a "non-mixing" basis and are treated here :
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C -----------------------------------------------------------------------------------
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IF(l==0) THEN
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IF (nsp==1) THEN
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Dmat(1,iorb)%mat(1,1) =
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& ( Dmat(1,iorb)%mat(1,1)+
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& CONJG(Dmat(1,iorb)%mat(1,1)) )/2.d0
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ELSE
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ALLOCATE(tmp_mat(1,1,nsp))
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tmp_mat=0.d0
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C Application of the time-reversal operation
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C ------------------------------------------
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DO is=1,nsp
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is1=is+(-1)**(is+1)
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C the time reversal operation transforms up/up -1- in dn/dn -2- and up/dn -3- in dn/up -4- (and vice versa)
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tmp_mat(1,1,is)=CONJG(Dmat(is1,iorb)%mat(1,1) )
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IF (is.gt.2) tmp_mat(1,1,is)=-tmp_mat(1,1,is)
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C Off diagonal blocks are multiplied by (-1).
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ENDDO
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C Symmetrization of Dmat :
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C ------------------------
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DO is=1,nsp
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Dmat(is,iorb)%mat(1,1) = (Dmat(is,iorb)%mat(1,1)+
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& tmp_mat(1,1,is) )/2.d0
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ENDDO
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DEALLOCATE(tmp_mat)
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ENDIF
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C -----------------------------------------------------------------------------------------------------
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C If the basis representation needs a complete spinor rotation approach (matrices of size 2*(2*l+1) ) :
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C -----------------------------------------------------------------------------------------------------
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ELSEIF (reptrans(l,isrt)%ifmixing) THEN
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C Calculation of the time-reversal operator :
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C -------------------------------------------
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ALLOCATE(time_op(1:2*(2*l+1),1:2*(2*l+1)))
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time_op(:,:)=0.d0
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DO m=1,2*(2*l+1)
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time_op(m,m)=1.d0
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ENDDO
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C time_op is Identity.
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CALL timeinv_op(time_op,2*(2*l+1),l,isrt)
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C time_op is now the time-reversal operator in the desired basis ({new_i})
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C
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C Application of the time-reversal operation
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C ------------------------------------------
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ALLOCATE(tmp_mat(1:2*(2*l+1),1:2*(2*l+1),1))
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tmp_mat(1:2*(2*l+1),1:2*(2*l+1),1)=
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= MATMUL(Dmat(1,iorb)%mat(1:2*(2*l+1),1:2*(2*l+1)),
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& TRANSPOSE(time_op(1:2*(2*l+1),1:2*(2*l+1)) ) )
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tmp_mat(1:2*(2*l+1),1:2*(2*l+1),1)=
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= MATMUL(time_op(1:2*(2*l+1),1:2*(2*l+1)),
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& CONJG(tmp_mat(1:2*(2*l+1),1:2*(2*l+1),1) ) )
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C The operation performed is : time_op.conjugate(Dmat).transpose(conjugate(time_op))
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C or in other words, D(T)_{new_i} . Dmat* . D(inverse(T))*_{new_i}
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C
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C Symmetrization of Dmat :
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C ------------------------
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Dmat(1,iorb)%mat(1:2*(2*l+1),1:2*(2*l+1)) =
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& ( Dmat(1,iorb)%mat(1:2*(2*l+1),1:2*(2*l+1)) +
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& tmp_mat(1:2*(2*l+1),1:2*(2*l+1),1) )/2.d0
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DEALLOCATE(tmp_mat)
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DEALLOCATE(time_op)
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C ----------------------------------------------------------------------------------------------
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C If the basis representation can be reduce to the up/up block (matrices of size (2*l+1) only) :
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C ----------------------------------------------------------------------------------------------
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ELSE
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C Calculation of the time-reversal operator :
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C -------------------------------------------
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ALLOCATE(time_op(-l:l,-l:l))
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time_op(:,:)=0.d0
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DO m=-l,l
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time_op(m,m)=1.d0
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ENDDO
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C time_op is Identity.
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CALL timeinv_op(time_op,(2*l+1),l,isrt)
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C time_op is now the time-reversal operator in the desired basis ({new_i})
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C
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IF (nsp==1) THEN
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C Application of the time-reversal operation and symmetrization :
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C ---------------------------------------------------------------
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ALLOCATE(tmp_mat(-l:l,-l:l,1))
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tmp_mat(-l:l,-l:l,1)=
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= MATMUL( Dmat(1,iorb)%mat(-l:l,-l:l),
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& TRANSPOSE(time_op(-l:l,-l:l) ) )
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tmp_mat(-l:l,-l:l,1)=
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= MATMUL(time_op(-l:l,-l:l),
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& CONJG(tmp_mat(-l:l,-l:l,1)) )
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C The operation performed is : time_op.conjugate(Dmat).transpose(conjugate(time_op))
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C or in other words, D(T)_{new_i} . Dmat* . D(inverse(T))*_{new_i}
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Dmat(1,iorb)%mat(-l:l,-l:l) =
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& ( Dmat(1,iorb)%mat(-l:l,-l:l) +
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& tmp_mat(-l:l,-l:l,1) )/2.d0
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DEALLOCATE(tmp_mat)
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ELSE
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C Application of the time-reversal operation
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C ------------------------------------------
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ALLOCATE(tmp_mat(-l:l,-l:l,nsp))
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DO is=1,nsp
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is1=is+(-1)**(is+1)
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C the time reversal operation transforms up/up -1- in dn/dn -2- and up/dn -3- in dn/up -4 (and vice versa)
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tmp_mat(-l:l,-l:l,is)=
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= MATMUL( Dmat(is1,iorb)%mat(-l:l,-l:l),
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& TRANSPOSE( time_op(-l:l,-l:l) ) )
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tmp_mat(-l:l,-l:l,is)=
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= MATMUL( time_op(-l:l,-l:l),
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& CONJG( tmp_mat(-l:l,-l:l,is) ) )
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C The operation performed is : time_op.conjugate(Dmat).transpose(conjugate(time_op))
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C or in other words, D(T)_{new_i} . Dmat* . D(inverse(T))*_{new_i}
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IF (is.gt.2) THEN
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tmp_mat(-l:l,-l:l,is)=-tmp_mat(-l:l,-l:l,is)
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ENDIF
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C Off diagonal terms are multiplied by (-1).
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ENDDO
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C Symmetrization of Dmat :
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C ------------------------
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DO is=1,nsp
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Dmat(is,iorb)%mat(-l:l,-l:l) =
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& (Dmat(is,iorb)%mat(-l:l,-l:l)+
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& tmp_mat(-l:l,-l:l,is) )/2.d0
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ENDDO
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DEALLOCATE(tmp_mat)
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ENDIF
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DEALLOCATE(time_op)
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C
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ENDIF ! End of the type basis if-then-else
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ENDDO ! End of the iorb loop
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C
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RETURN
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END
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