mirror of
https://github.com/pfloos/quack
synced 2024-10-31 19:23:52 +01:00
GIC functional
This commit is contained in:
parent
5a80b38685
commit
192a6345de
@ -18,6 +18,5 @@
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double precision,parameter :: CxLDA = - (3d0/4d0)*(3d0/pi)**(1d0/3d0)
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double precision,parameter :: Cx0 = - (4d0/3d0)*(1d0/pi)**(1d0/3d0)
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! double precision,parameter :: Cx1 = - 0.913d0*(4d0/3d0)*(1d0/pi)**(1d0/3d0)
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double precision,parameter :: Cx1 = - (176d0/105d0)*(1d0/pi)**(1d0/3d0)
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48
input/basis
48
input/basis
@ -1,27 +1,43 @@
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1 5
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1 9
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S 3
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1 13.0100000 0.0196850
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2 1.9620000 0.1379770
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3 0.4446000 0.4781480
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1 33.8700000 0.0060680
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2 5.0950000 0.0453080
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3 1.1590000 0.2028220
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S 1
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1 0.1220000 1.0000000
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1 0.3258000 1.0000000
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S 1
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1 0.0297400 1.0000000
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1 0.1027000 1.0000000
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S 1
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1 0.0252600 1.0000000
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P 1
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1 0.7270000 1.0000000
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1 1.4070000 1.0000000
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P 1
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1 0.1410000 1.0000000
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2 5
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1 0.3880000 1.0000000
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P 1
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1 0.1020000 1.0000000
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D 1
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1 1.0570000 1.0000000
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D 1
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1 0.2470000 1.0000000
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2 9
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S 3
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1 13.0100000 0.0196850
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2 1.9620000 0.1379770
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3 0.4446000 0.4781480
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1 33.8700000 0.0060680
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2 5.0950000 0.0453080
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3 1.1590000 0.2028220
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S 1
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1 0.1220000 1.0000000
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1 0.3258000 1.0000000
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S 1
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1 0.0297400 1.0000000
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1 0.1027000 1.0000000
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S 1
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1 0.0252600 1.0000000
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P 1
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1 0.7270000 1.0000000
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1 1.4070000 1.0000000
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P 1
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1 0.1410000 1.0000000
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1 0.3880000 1.0000000
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P 1
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1 0.1020000 1.0000000
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D 1
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1 1.0570000 1.0000000
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D 1
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1 0.2470000 1.0000000
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@ -2,11 +2,11 @@
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GOK-RKS
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# exchange rung:
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# Hartree = 0
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# LDA = 1: RS51,RMFL20
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# LDA = 1: RS51,RMFL20,RGIC
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# GGA = 2: RB88
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# Hybrid = 4
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# Hartree-Fock = 666
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666 HF
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1 RGIC
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# correlation rung:
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# Hartree = 0
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# LDA = 1: RVWN5,RMFL20
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48
input/weight
48
input/weight
@ -1,27 +1,43 @@
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1 5
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1 9
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S 3
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1 13.0100000 0.0196850
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2 1.9620000 0.1379770
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3 0.4446000 0.4781480
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1 33.8700000 0.0060680
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2 5.0950000 0.0453080
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3 1.1590000 0.2028220
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S 1
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1 0.1220000 1.0000000
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1 0.3258000 1.0000000
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S 1
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1 0.0297400 1.0000000
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1 0.1027000 1.0000000
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S 1
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1 0.0252600 1.0000000
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P 1
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1 0.7270000 1.0000000
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1 1.4070000 1.0000000
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P 1
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1 0.1410000 1.0000000
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2 5
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1 0.3880000 1.0000000
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P 1
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1 0.1020000 1.0000000
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D 1
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1 1.0570000 1.0000000
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D 1
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1 0.2470000 1.0000000
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2 9
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S 3
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1 13.0100000 0.0196850
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2 1.9620000 0.1379770
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3 0.4446000 0.4781480
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1 33.8700000 0.0060680
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2 5.0950000 0.0453080
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3 1.1590000 0.2028220
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S 1
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1 0.1220000 1.0000000
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1 0.3258000 1.0000000
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S 1
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1 0.0297400 1.0000000
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1 0.1027000 1.0000000
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S 1
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1 0.0252600 1.0000000
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P 1
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1 0.7270000 1.0000000
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1 1.4070000 1.0000000
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P 1
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1 0.1410000 1.0000000
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1 0.3880000 1.0000000
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P 1
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1 0.1020000 1.0000000
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D 1
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1 1.0570000 1.0000000
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D 1
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1 0.2470000 1.0000000
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@ -45,6 +45,7 @@ subroutine G0T0(doACFDT,exchange_kernel,doXBS,BSE,TDA,singlet_manifold,triplet_m
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double precision,allocatable :: X2s(:,:),X2t(:,:)
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double precision,allocatable :: Y2s(:,:),Y2t(:,:)
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double precision,allocatable :: rho2s(:,:,:),rho2t(:,:,:)
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double precision,allocatable :: rho1st(:,:,:),rho2st(:,:,:)
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double precision,allocatable :: SigT(:)
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double precision,allocatable :: Z(:)
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@ -81,6 +82,7 @@ subroutine G0T0(doACFDT,exchange_kernel,doXBS,BSE,TDA,singlet_manifold,triplet_m
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Omega1t(nVVt),X1t(nVVt,nVVt),Y1t(nOOt,nVVt), &
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Omega2t(nOOt),X2t(nVVt,nOOt),Y2t(nOOt,nOOt), &
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rho1t(nBas,nO,nVVt),rho2t(nBas,nV,nOOt), &
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rho1st(nBas,nO,nVVt),rho2st(nBas,nV,nOOt), &
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SigT(nBas),Z(nBas),eG0T0(nBas))
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!----------------------------------------------
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@ -100,14 +102,6 @@ subroutine G0T0(doACFDT,exchange_kernel,doXBS,BSE,TDA,singlet_manifold,triplet_m
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call print_excitation('pp-RPA (N+2)',ispin,nVVs,Omega1s(:))
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call print_excitation('pp-RPA (N-2)',ispin,nOOs,Omega2s(:))
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! Compute excitation densities for the T-matrix
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rho1s(:,:,:) = 0d0
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rho2s(:,:,:) = 0d0
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call excitation_density_Tmatrix(ispin,1d0,nBas,nC,nO,nV,nR,nOOs,nVVs,ERI(:,:,:,:), &
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X1s(:,:),Y1s(:,:),rho1s(:,:,:),X2s(:,:),Y2s(:,:),rho2s(:,:,:))
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!----------------------------------------------
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! Triplet manifold
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!----------------------------------------------
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@ -125,72 +119,33 @@ subroutine G0T0(doACFDT,exchange_kernel,doXBS,BSE,TDA,singlet_manifold,triplet_m
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call print_excitation('pp-RPA (N+2)',ispin,nVVt,Omega1t(:))
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call print_excitation('pp-RPA (N-2)',ispin,nOOt,Omega2t(:))
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! Compute excitation densities for the T-matrix
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!-----------------------------------------------------------
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! Compute excitation densities for the T-matrix self-energy
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!-----------------------------------------------------------
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rho1t(:,:,:) = 0d0
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rho2t(:,:,:) = 0d0
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call excitation_density_Tmatrix(ispin,1d0,nBas,nC,nO,nV,nR,nOOt,nVVt,ERI(:,:,:,:), &
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call excitation_density_Tmatrix(nBas,nC,nO,nV,nR,nOOs,nVVs,nOOt,nVVt,ERI(:,:,:,:),rho1st(:,:,:),rho2st(:,:,:), &
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X1s(:,:),Y1s(:,:),rho1s(:,:,:),X2s(:,:),Y2s(:,:),rho2s(:,:,:), &
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X1t(:,:),Y1t(:,:),rho1t(:,:,:),X2t(:,:),Y2t(:,:),rho2t(:,:,:))
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!----------------------------------------------
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! Compute T-matrix version of the self-energy
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!----------------------------------------------
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SigT(:) = 0d0
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rho2s(:,:,:) = 0d0
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rho2t(:,:,:) = 0d0
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! rho2s(:,:,:) = 0d0
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! rho2t(:,:,:) = 0d0
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! rho2st(:,:,:) = 0d0
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call self_energy_Tmatrix_diag(eta,nBas,nC,nO,nV,nR,nOOs,nVVs,nOOt,nVVt,eHF(:), &
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Omega1s(:),rho1s(:,:,:),Omega2s(:),rho2s(:,:,:), &
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Omega1t(:),rho1t(:,:,:),Omega2t(:),rho2t(:,:,:), &
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SigT(:))
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!----------------------------------------------
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! Singlet manifold
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!----------------------------------------------
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ispin = 1
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! Compute excitation densities for the T-matrix
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rho1s(:,:,:) = 0d0
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rho2s(:,:,:) = 0d0
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call excitation_density_Tmatrix(ispin,0d0,nBas,nC,nO,nV,nR,nOOs,nVVs,ERI(:,:,:,:), &
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X1s(:,:),Y1s(:,:),rho1s(:,:,:),X2s(:,:),Y2s(:,:),rho2s(:,:,:))
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!----------------------------------------------
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! Triplet manifold
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!----------------------------------------------
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ispin = 2
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! Compute excitation densities for the T-matrix
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rho1t(:,:,:) = 0d0
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rho2t(:,:,:) = 0d0
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call excitation_density_Tmatrix(ispin,0d0,nBas,nC,nO,nV,nR,nOOt,nVVt,ERI(:,:,:,:), &
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X1t(:,:),Y1t(:,:),rho1t(:,:,:),X2t(:,:),Y2t(:,:),rho2t(:,:,:))
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!----------------------------------------------
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! Compute T-matrix version of the self-energy
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!----------------------------------------------
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rho2s(:,:,:) = 0d0
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rho2t(:,:,:) = 0d0
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call self_energy_Tmatrix_diag(eta,nBas,nC,nO,nV,nR,nOOs,nVVs,nOOt,nVVt,eHF(:), &
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Omega1s(:),rho1s(:,:,:),Omega2s(:),rho2s(:,:,:), &
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Omega1t(:),rho1t(:,:,:),Omega2t(:),rho2t(:,:,:), &
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SigT(:))
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rho1st(:,:,:),rho2st(:,:,:),SigT(:))
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! Compute renormalization factor for T-matrix self-energy
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call renormalization_factor_Tmatrix(eta,nBas,nC,nO,nV,nR,nOOs,nVVs,nOOt,nVVt,eHF(:), &
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Omega1s(:),rho1s(:,:,:),Omega2s(:),rho2s(:,:,:), &
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Omega1t(:),rho1t(:,:,:),Omega2t(:),rho2t(:,:,:), &
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Z(:))
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rho1st(:,:,:),rho2st(:,:,:),Z(:))
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!----------------------------------------------
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! Solve the quasi-particle equation
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@ -1,4 +1,5 @@
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subroutine excitation_density_Tmatrix(ispin,db,nBas,nC,nO,nV,nR,nOO,nVV,ERI,X1,Y1,rho1,X2,Y2,rho2)
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subroutine excitation_density_Tmatrix(nBas,nC,nO,nV,nR,nOOs,nVVs,nOOt,nVVt,ERI,rho1st,rho2st, &
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X1s,Y1s,rho1s,X2s,Y2s,rho2s,X1t,Y1t,rho1t,X2t,Y2t,rho2t)
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! Compute excitation densities for T-matrix self-energy
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@ -6,14 +7,24 @@ subroutine excitation_density_Tmatrix(ispin,db,nBas,nC,nO,nV,nR,nOO,nVV,ERI,X1,Y
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! Input variables
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integer,intent(in) :: ispin
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double precision,intent(in) :: db
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integer,intent(in) :: nBas,nC,nO,nV,nR,nOO,nVV
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integer,intent(in) :: nBas
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integer,intent(in) :: nC
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integer,intent(in) :: nO
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integer,intent(in) :: nV
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integer,intent(in) :: nR
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double precision,intent(in) :: ERI(nBas,nBas,nBas,nBas)
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double precision,intent(in) :: X1(nVV,nVV)
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double precision,intent(in) :: Y1(nOO,nVV)
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double precision,intent(in) :: X2(nVV,nOO)
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double precision,intent(in) :: Y2(nOO,nOO)
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integer,intent(in) :: nOOs
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integer,intent(in) :: nOOt
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double precision,intent(in) :: X1s(nVVs,nVVs)
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double precision,intent(in) :: Y1s(nOOs,nVVs)
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double precision,intent(in) :: X2s(nVVs,nOOs)
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double precision,intent(in) :: Y2s(nOOs,nOOs)
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integer,intent(in) :: nVVs
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integer,intent(in) :: nVVt
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double precision,intent(in) :: X1t(nVVt,nVVt)
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double precision,intent(in) :: Y1t(nOOt,nVVt)
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double precision,intent(in) :: X2t(nVVt,nOOt)
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double precision,intent(in) :: Y2t(nOOt,nOOt)
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! Local variables
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@ -25,187 +36,176 @@ subroutine excitation_density_Tmatrix(ispin,db,nBas,nC,nO,nV,nR,nOO,nVV,ERI,X1,Y
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! Output variables
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double precision,intent(out) :: rho1(nBas,nO,nVV)
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double precision,intent(out) :: rho2(nBas,nV,nOO)
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double precision,intent(out) :: rho1s(nBas,nO,nVVs)
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double precision,intent(out) :: rho2s(nBas,nV,nOOs)
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double precision,intent(out) :: rho1t(nBas,nO,nVVt)
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double precision,intent(out) :: rho2t(nBas,nV,nOOt)
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double precision,intent(out) :: rho1st(nBas,nO,nVVt)
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double precision,intent(out) :: rho2st(nBas,nV,nOOt)
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! Initialization
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rho1s(:,:,:) = 0d0
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rho2s(:,:,:) = 0d0
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rho1t(:,:,:) = 0d0
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rho2t(:,:,:) = 0d0
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rho1st(:,:,:) = 0d0
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rho2st(:,:,:) = 0d0
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!----------------------------------------------
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! Singlet manifold
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!----------------------------------------------
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if(ispin == 1) then
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do p=nC+1,nBas-nR
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do p=nC+1,nBas-nR
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do i=nC+1,nO
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do ab=1,nVVs
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do i=nC+1,nO
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do ab=1,nVV
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cd = 0
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do c=nO+1,nBas-nR
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do d=c,nBas-nR
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cd = cd + 1
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rho1(p,i,ab) = rho1(p,i,ab) &
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! + db*(ERI(p,i,c,d) + ERI(p,i,d,c))*X1(cd,ab) &
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! /sqrt((1d0 + Kronecker_delta(p,i))*(1d0 + Kronecker_delta(c,d))) &
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+ 0d0*db*(ERI(p,i,c,d) - ERI(p,i,d,c))*X1(cd,ab) &
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+ (1d0 - db)*ERI(p,i,c,d)*X1(cd,ab)
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end do
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cd = 0
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do c=nO+1,nBas-nR
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do d=c,nBas-nR
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cd = cd + 1
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rho1s(p,i,ab) = rho1s(p,i,ab) + 2.0d0*ERI(p,i,c,d)*X1s(cd,ab)
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end do
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kl = 0
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do k=nC+1,nO
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do l=k,nO
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kl = kl + 1
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rho1(p,i,ab) = rho1(p,i,ab) &
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! + db*(ERI(p,i,k,l) + ERI(p,i,l,k))*Y1(kl,ab) &
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! /sqrt((1d0 + Kronecker_delta(p,i))*(1d0 + Kronecker_delta(k,l))) &
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+ 0d0*db*(ERI(p,i,k,l) - ERI(p,i,l,k))*Y1(kl,ab) &
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+ (1d0 - db)*ERI(p,i,k,l)*Y1(kl,ab)
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end do
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end do
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end do
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end do
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do a=1,nV-nR
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do ij=1,nOO
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cd = 0
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do c=nO+1,nBas-nR
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do d=c,nBas-nR
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cd = cd + 1
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rho2(p,a,ij) = rho2(p,a,ij) + db*(ERI(p,nO+a,c,d) - ERI(p,nO+a,d,c))*X2(cd,ij)
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end do
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kl = 0
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do k=nC+1,nO
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do l=k,nO
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kl = kl + 1
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rho1s(p,i,ab) = rho1s(p,i,ab) + 2.0d0*ERI(p,i,k,l)*Y1s(kl,ab)
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end do
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kl = 0
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do k=nC+1,nO
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do l=k,nO
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kl = kl + 1
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rho2(p,a,ij) = rho2(p,a,ij) + db*(ERI(p,nO+a,k,l) - ERI(p,nO+a,l,k))*Y2(kl,ij)
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end do
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end do
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end do
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end do
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end do
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end do
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end if
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do a=1,nV-nR
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do ij=1,nOOs
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cd = 0
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do c=nO+1,nBas-nR
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do d=c,nBas-nR
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cd = cd + 1
|
||||
rho2s(p,a,ij) = rho2s(p,a,ij) + 2.0d0*ERI(p,nO+a,c,d)*X2s(cd,ij)
|
||||
end do
|
||||
end do
|
||||
|
||||
kl = 0
|
||||
do k=nC+1,nO
|
||||
do l=k,nO
|
||||
kl = kl + 1
|
||||
rho2s(p,a,ij) = rho2s(p,a,ij) + 2.0d0*ERI(p,nO+a,k,l)*Y2s(kl,ij)
|
||||
end do
|
||||
end do
|
||||
|
||||
end do
|
||||
end do
|
||||
|
||||
end do
|
||||
|
||||
!----------------------------------------------
|
||||
! Triplet manifold
|
||||
!----------------------------------------------
|
||||
|
||||
if(ispin == 2) then
|
||||
do p=nC+1,nBas-nR
|
||||
|
||||
do p=nC+1,nBas-nR
|
||||
do i=nC+1,nO
|
||||
do ab=1,nVVt
|
||||
|
||||
do i=nC+1,nO
|
||||
do ab=1,nVV
|
||||
|
||||
cd = 0
|
||||
do c=nO+1,nBas-nR
|
||||
do d=c+1,nBas-nR
|
||||
cd = cd + 1
|
||||
rho1(p,i,ab) = rho1(p,i,ab) &
|
||||
+ 1.0d0*db*(ERI(p,i,c,d) - ERI(p,i,d,c))*X1(cd,ab) &
|
||||
+ (1d0-db)*0d0*(ERI(p,i,c,d))*X1(cd,ab)
|
||||
end do
|
||||
cd = 0
|
||||
do c=nO+1,nBas-nR
|
||||
do d=c+1,nBas-nR
|
||||
cd = cd + 1
|
||||
rho1t(p,i,ab) = rho1t(p,i,ab) + 1d0*(ERI(p,i,c,d) - ERI(p,i,d,c))*X1t(cd,ab)
|
||||
end do
|
||||
|
||||
kl = 0
|
||||
do k=nC+1,nO
|
||||
do l=k+1,nO
|
||||
kl = kl + 1
|
||||
rho1(p,i,ab) = rho1(p,i,ab) &
|
||||
+ 1.0d0*db*(ERI(p,i,k,l) - ERI(p,i,l,k))*Y1(kl,ab) &
|
||||
+ (1d0-db)*0d0*(ERI(p,i,k,l))*Y1(kl,ab)
|
||||
end do
|
||||
end do
|
||||
|
||||
end do
|
||||
end do
|
||||
|
||||
do a=1,nV-nR
|
||||
do ij=1,nOO
|
||||
|
||||
cd = 0
|
||||
do c=nO+1,nBas-nR
|
||||
do d=c+1,nBas-nR
|
||||
cd = cd + 1
|
||||
rho2(p,a,ij) = rho2(p,a,ij) + 1d0*(ERI(p,nO+a,c,d) - db*ERI(p,nO+a,d,c))*X2(cd,ij)
|
||||
end do
|
||||
kl = 0
|
||||
do k=nC+1,nO
|
||||
do l=k+1,nO
|
||||
kl = kl + 1
|
||||
rho1t(p,i,ab) = rho1t(p,i,ab) + 1d0*(ERI(p,i,k,l) - ERI(p,i,l,k))*Y1t(kl,ab)
|
||||
end do
|
||||
|
||||
kl = 0
|
||||
do k=nC+1,nO
|
||||
do l=k+1,nO
|
||||
kl = kl + 1
|
||||
rho2(p,a,ij) = rho2(p,a,ij) + 1d0*(ERI(p,nO+a,k,l) - db*ERI(p,nO+a,l,k))*Y2(kl,ij)
|
||||
end do
|
||||
end do
|
||||
|
||||
end do
|
||||
end do
|
||||
|
||||
end do
|
||||
end do
|
||||
|
||||
end if
|
||||
do a=1,nV-nR
|
||||
do ij=1,nOOt
|
||||
|
||||
!----------------------------------------------
|
||||
! Spinorbital basis
|
||||
!----------------------------------------------
|
||||
|
||||
if(ispin == 3) then
|
||||
|
||||
do p=nC+1,nBas-nR
|
||||
|
||||
do i=nC+1,nO
|
||||
do ab=1,nVV
|
||||
|
||||
cd = 0
|
||||
do c=nO+1,nBas-nR
|
||||
do d=c+1,nBas-nR
|
||||
cd = cd + 1
|
||||
rho1(p,i,ab) = rho1(p,i,ab) + (ERI(p,i,c,d) - ERI(p,i,d,c))*X1(cd,ab)
|
||||
end do
|
||||
cd = 0
|
||||
do c=nO+1,nBas-nR
|
||||
do d=c+1,nBas-nR
|
||||
cd = cd + 1
|
||||
rho2t(p,a,ij) = rho2t(p,a,ij) + 1d0*(ERI(p,nO+a,c,d) - ERI(p,nO+a,d,c))*X2t(cd,ij)
|
||||
end do
|
||||
|
||||
kl = 0
|
||||
do k=nC+1,nO
|
||||
do l=k+1,nO
|
||||
kl = kl + 1
|
||||
rho1(p,i,ab) = rho1(p,i,ab) + (ERI(p,i,k,l) - ERI(p,i,l,k))*Y1(kl,ab)
|
||||
end do
|
||||
end do
|
||||
|
||||
end do
|
||||
end do
|
||||
|
||||
do a=1,nV-nR
|
||||
do ij=1,nOO
|
||||
|
||||
cd = 0
|
||||
do c=nO+1,nBas-nR
|
||||
do d=c+1,nBas-nR
|
||||
cd = cd + 1
|
||||
rho2(p,a,ij) = rho2(p,a,ij) + (ERI(p,nO+a,c,d) - ERI(p,nO+a,d,c))*X2(cd,ij)
|
||||
end do
|
||||
kl = 0
|
||||
do k=nC+1,nO
|
||||
do l=k+1,nO
|
||||
kl = kl + 1
|
||||
rho2t(p,a,ij) = rho2t(p,a,ij) + 1d0*(ERI(p,nO+a,k,l) - ERI(p,nO+a,l,k))*Y2t(kl,ij)
|
||||
end do
|
||||
|
||||
kl = 0
|
||||
do k=nC+1,nO
|
||||
do l=k+1,nO
|
||||
kl = kl + 1
|
||||
rho2(p,a,ij) = rho2(p,a,ij) + (ERI(p,nO+a,k,l) - ERI(p,nO+a,l,k))*Y2(kl,ij)
|
||||
end do
|
||||
end do
|
||||
|
||||
end do
|
||||
end do
|
||||
|
||||
end do
|
||||
end do
|
||||
|
||||
end if
|
||||
end do
|
||||
|
||||
!----------------------------------------------
|
||||
! Singlet-triplet crossed term
|
||||
!----------------------------------------------
|
||||
|
||||
do p=nC+1,nBas-nR
|
||||
|
||||
do i=nC+1,nO
|
||||
do ab=1,nVVt
|
||||
|
||||
cd = 0
|
||||
do c=nO+1,nBas-nR
|
||||
do d=c+1,nBas-nR
|
||||
cd = cd + 1
|
||||
rho1st(p,i,ab) = rho1st(p,i,ab) + 2d0*ERI(p,i,c,d)*X1t(cd,ab)
|
||||
end do
|
||||
end do
|
||||
|
||||
kl = 0
|
||||
do k=nC+1,nO
|
||||
do l=k+1,nO
|
||||
kl = kl + 1
|
||||
rho1st(p,i,ab) = rho1st(p,i,ab) + 2d0*ERI(p,i,k,l)*Y1t(kl,ab)
|
||||
end do
|
||||
end do
|
||||
|
||||
end do
|
||||
end do
|
||||
|
||||
do a=1,nV-nR
|
||||
do ij=1,nOOt
|
||||
|
||||
cd = 0
|
||||
do c=nO+1,nBas-nR
|
||||
do d=c+1,nBas-nR
|
||||
cd = cd + 1
|
||||
rho2st(p,a,ij) = rho2st(p,a,ij) + 2d0*ERI(p,nO+a,c,d)*X2t(cd,ij)
|
||||
end do
|
||||
end do
|
||||
|
||||
kl = 0
|
||||
do k=nC+1,nO
|
||||
do l=k+1,nO
|
||||
kl = kl + 1
|
||||
rho2st(p,a,ij) = rho2st(p,a,ij) + 2d0*ERI(p,nO+a,k,l)*Y2t(kl,ij)
|
||||
end do
|
||||
end do
|
||||
|
||||
end do
|
||||
end do
|
||||
|
||||
end do
|
||||
|
||||
end subroutine excitation_density_Tmatrix
|
||||
|
82
src/QuAcK/excitation_density_Tmatrix_so.f90
Normal file
82
src/QuAcK/excitation_density_Tmatrix_so.f90
Normal file
@ -0,0 +1,82 @@
|
||||
subroutine excitation_density_Tmatrix_so(nBas,nC,nO,nV,nR,nOO,nVV,ERI,X1,Y1,rho1,X2,Y2,rho2)
|
||||
|
||||
! Compute excitation densities for T-matrix self-energy
|
||||
|
||||
implicit none
|
||||
|
||||
! Input variables
|
||||
|
||||
integer,intent(in) :: nBas,nC,nO,nV,nR,nOO,nVV
|
||||
double precision,intent(in) :: ERI(nBas,nBas,nBas,nBas)
|
||||
double precision,intent(in) :: X1(nVV,nVV)
|
||||
double precision,intent(in) :: Y1(nOO,nVV)
|
||||
double precision,intent(in) :: X2(nVV,nOO)
|
||||
double precision,intent(in) :: Y2(nOO,nOO)
|
||||
|
||||
! Local variables
|
||||
|
||||
integer :: i,j,k,l
|
||||
integer :: a,b,c,d
|
||||
integer :: p
|
||||
integer :: ab,cd,ij,kl
|
||||
double precision,external :: Kronecker_delta
|
||||
|
||||
! Output variables
|
||||
|
||||
double precision,intent(out) :: rho1(nBas,nO,nVV)
|
||||
double precision,intent(out) :: rho2(nBas,nV,nOO)
|
||||
|
||||
! Initialization
|
||||
|
||||
rho1(:,:,:) = 0d0
|
||||
rho2(:,:,:) = 0d0
|
||||
|
||||
do p=nC+1,nBas-nR
|
||||
|
||||
do i=nC+1,nO
|
||||
do ab=1,nVV
|
||||
|
||||
cd = 0
|
||||
do c=nO+1,nBas-nR
|
||||
do d=c+1,nBas-nR
|
||||
cd = cd + 1
|
||||
rho1(p,i,ab) = rho1(p,i,ab) + (ERI(p,i,c,d) - ERI(p,i,d,c))*X1(cd,ab)
|
||||
end do
|
||||
end do
|
||||
|
||||
kl = 0
|
||||
do k=nC+1,nO
|
||||
do l=k+1,nO
|
||||
kl = kl + 1
|
||||
rho1(p,i,ab) = rho1(p,i,ab) + (ERI(p,i,k,l) - ERI(p,i,l,k))*Y1(kl,ab)
|
||||
end do
|
||||
end do
|
||||
|
||||
end do
|
||||
end do
|
||||
|
||||
do a=1,nV-nR
|
||||
do ij=1,nOO
|
||||
|
||||
cd = 0
|
||||
do c=nO+1,nBas-nR
|
||||
do d=c+1,nBas-nR
|
||||
cd = cd + 1
|
||||
rho2(p,a,ij) = rho2(p,a,ij) + (ERI(p,nO+a,c,d) - ERI(p,nO+a,d,c))*X2(cd,ij)
|
||||
end do
|
||||
end do
|
||||
|
||||
kl = 0
|
||||
do k=nC+1,nO
|
||||
do l=k+1,nO
|
||||
kl = kl + 1
|
||||
rho2(p,a,ij) = rho2(p,a,ij) + (ERI(p,nO+a,k,l) - ERI(p,nO+a,l,k))*Y2(kl,ij)
|
||||
end do
|
||||
end do
|
||||
|
||||
end do
|
||||
end do
|
||||
|
||||
end do
|
||||
|
||||
end subroutine excitation_density_Tmatrix_so
|
@ -49,8 +49,6 @@ subroutine linear_response_A_matrix(ispin,dRPA,nBas,nC,nO,nV,nR,nS,lambda,e,ERI,
|
||||
A_lr(ia,jb) = (e(a) - e(i))*Kronecker_delta(i,j)*Kronecker_delta(a,b) &
|
||||
+ (1d0 + delta_spin)*lambda*ERI(i,b,a,j) &
|
||||
- (1d0 - delta_dRPA)*lambda*ERI(i,b,j,a)
|
||||
! + (1d0 + delta_spin)*lambda*ERI(i,j,a,b) &
|
||||
! - (1d0 - delta_dRPA)*lambda*ERI(i,a,j,b)
|
||||
|
||||
enddo
|
||||
enddo
|
||||
|
@ -46,8 +46,6 @@ subroutine linear_response_B_matrix(ispin,dRPA,nBas,nC,nO,nV,nR,nS,lambda,ERI,B_
|
||||
|
||||
B_lr(ia,jb) = (1d0 + delta_spin)*lambda*ERI(i,j,a,b) &
|
||||
- (1d0 - delta_dRPA)*lambda*ERI(i,j,b,a)
|
||||
! B_lr(ia,jb) = (1d0 + delta_spin)*lambda*ERI(i,b,a,j) &
|
||||
! - (1d0 - delta_dRPA)*lambda*ERI(i,a,b,j)
|
||||
|
||||
enddo
|
||||
enddo
|
||||
|
@ -1,6 +1,6 @@
|
||||
subroutine renormalization_factor_Tmatrix(eta,nBas,nC,nO,nV,nR,nOOs,nVVs,nOOt,nVVt,e, &
|
||||
Omega1s,rho1s,Omega2s,rho2s,Omega1t,rho1t,Omega2t,rho2t, &
|
||||
Z)
|
||||
rho1st,rho2st,Z)
|
||||
|
||||
! Compute renormalization factor of the T-matrix self-energy
|
||||
|
||||
@ -15,9 +15,9 @@ subroutine renormalization_factor_Tmatrix(eta,nBas,nC,nO,nV,nR,nOOs,nVVs,nOOt,nV
|
||||
integer,intent(in) :: nVVs,nVVt
|
||||
double precision,intent(in) :: e(nBas)
|
||||
double precision,intent(in) :: Omega1s(nVVs),Omega1t(nVVt)
|
||||
double precision,intent(in) :: rho1s(nBas,nO,nVVs),rho1t(nBas,nO,nVVt)
|
||||
double precision,intent(in) :: rho1s(nBas,nO,nVVs),rho1t(nBas,nO,nVVt),rho1st(nBas,nO,nVVt)
|
||||
double precision,intent(in) :: Omega2s(nOOs),Omega2t(nOOt)
|
||||
double precision,intent(in) :: rho2s(nBas,nV,nOOs),rho2t(nBas,nV,nOOt)
|
||||
double precision,intent(in) :: rho2s(nBas,nV,nOOs),rho2t(nBas,nV,nOOt),rho2st(nBas,nV,nOOt)
|
||||
|
||||
! Local variables
|
||||
|
||||
@ -69,6 +69,7 @@ subroutine renormalization_factor_Tmatrix(eta,nBas,nC,nO,nV,nR,nOOs,nVVs,nOOt,nV
|
||||
do cd=1,nVVt
|
||||
eps = e(p) + e(i) - Omega1t(cd)
|
||||
Z(p) = Z(p) + (rho1t(p,i,cd)/eps)**2
|
||||
Z(p) = Z(p) + (rho1st(p,i,cd)/eps)**2
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
@ -80,6 +81,7 @@ subroutine renormalization_factor_Tmatrix(eta,nBas,nC,nO,nV,nR,nOOs,nVVs,nOOt,nV
|
||||
do kl=1,nOOt
|
||||
eps = e(p) + e(nO+a) - Omega2t(kl)
|
||||
Z(p) = Z(p) + (rho2t(p,a,kl)/eps)**2
|
||||
Z(p) = Z(p) + (rho2st(p,a,kl)/eps)**2
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
|
@ -1,6 +1,6 @@
|
||||
subroutine self_energy_Tmatrix_diag(eta,nBas,nC,nO,nV,nR,nOOs,nVVs,nOOt,nVVt,e, &
|
||||
Omega1s,rho1s,Omega2s,rho2s,Omega1t,rho1t,Omega2t,rho2t, &
|
||||
SigT)
|
||||
rho1st,rho2st,SigT)
|
||||
|
||||
! Compute diagonal of the correlation part of the T-matrix self-energy
|
||||
|
||||
@ -19,9 +19,9 @@ subroutine self_energy_Tmatrix_diag(eta,nBas,nC,nO,nV,nR,nOOs,nVVs,nOOt,nVVt,e,
|
||||
integer,intent(in) :: nVVs,nVVt
|
||||
double precision,intent(in) :: e(nBas)
|
||||
double precision,intent(in) :: Omega1s(nVVs),Omega1t(nVVt)
|
||||
double precision,intent(in) :: rho1s(nBas,nO,nVVs),rho1t(nBas,nO,nVVt)
|
||||
double precision,intent(in) :: rho1s(nBas,nO,nVVs),rho1t(nBas,nO,nVVt),rho1st(nBas,nO,nVVt)
|
||||
double precision,intent(in) :: Omega2s(nOOs),Omega2t(nOOt)
|
||||
double precision,intent(in) :: rho2s(nBas,nV,nOOs),rho2t(nBas,nV,nOOt)
|
||||
double precision,intent(in) :: rho2s(nBas,nV,nOOs),rho2t(nBas,nV,nOOt),rho2st(nBas,nV,nOOt)
|
||||
|
||||
! Local variables
|
||||
|
||||
@ -32,6 +32,10 @@ subroutine self_energy_Tmatrix_diag(eta,nBas,nC,nO,nV,nR,nOOs,nVVs,nOOt,nVVt,e,
|
||||
|
||||
double precision,intent(out) :: SigT(nBas)
|
||||
|
||||
! Initialization
|
||||
|
||||
SigT(:) = 0d0
|
||||
|
||||
!----------------------------------------------
|
||||
! Singlet part of the T-matrix self-energy
|
||||
!----------------------------------------------
|
||||
@ -69,6 +73,7 @@ subroutine self_energy_Tmatrix_diag(eta,nBas,nC,nO,nV,nR,nOOs,nVVs,nOOt,nVVt,e,
|
||||
do cd=1,nVVt
|
||||
eps = e(p) + e(i) - Omega1t(cd)
|
||||
SigT(p) = SigT(p) + rho1t(p,i,cd)**2/eps
|
||||
SigT(p) = SigT(p) + rho1st(p,i,cd)**2/eps
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
@ -80,6 +85,7 @@ subroutine self_energy_Tmatrix_diag(eta,nBas,nC,nO,nV,nR,nOOs,nVVs,nOOt,nVVt,e,
|
||||
do kl=1,nOOt
|
||||
eps = e(p) + e(nO+a) - Omega2t(kl)
|
||||
SigT(p) = SigT(p) + rho2t(p,a,kl)**2/eps
|
||||
SigT(p) = SigT(p) + rho2st(p,a,kl)**2/eps
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
|
@ -91,14 +91,14 @@ subroutine soG0T0(eta,nBas,nC,nO,nV,nR,ENuc,ERHF,ERI,eHF)
|
||||
rho1(:,:,:) = 0d0
|
||||
rho2(:,:,:) = 0d0
|
||||
|
||||
call excitation_density_Tmatrix(ispin,1d0,nBas2,nC2,nO2,nV2,nR2,nOO,nVV,sERI(:,:,:,:), &
|
||||
call excitation_density_Tmatrix_so(nBas2,nC2,nO2,nV2,nR2,nOO,nVV,sERI(:,:,:,:), &
|
||||
X1(:,:),Y1(:,:),rho1(:,:,:),X2(:,:),Y2(:,:),rho2(:,:,:))
|
||||
|
||||
!----------------------------------------------
|
||||
! Compute T-matrix version of the self-energy
|
||||
!----------------------------------------------
|
||||
|
||||
rho2(:,:,:) = 0d0
|
||||
! rho2(:,:,:) = 0d0
|
||||
|
||||
call self_energy_Tmatrix_diag_so(eta,nBas2,nC2,nO2,nV2,nR2,nOO,nVV,seHF(:), &
|
||||
Omega1(:),rho1(:,:,:),Omega2(:),rho2(:,:,:), &
|
||||
|
@ -3,7 +3,7 @@ BDIR =../../bin
|
||||
ODIR = obj
|
||||
OODIR = ../IntPak/obj
|
||||
SDIR =.
|
||||
FC = gfortran -I$(IDIR) -Wall
|
||||
FC = gfortran -I$(IDIR)
|
||||
ifeq ($(DEBUG),1)
|
||||
FFLAGS = -Wall -g -msse4.2 -fcheck=all -Waliasing -Wampersand -Wconversion -Wsurprising -Wintrinsics-std -Wno-tabs -Wintrinsic-shadow -Wline-truncation -Wreal-q-constant
|
||||
else
|
||||
|
65
src/eDFT/RGIC_lda_exchange_derivative_discontinuity.f90
Normal file
65
src/eDFT/RGIC_lda_exchange_derivative_discontinuity.f90
Normal file
@ -0,0 +1,65 @@
|
||||
subroutine RGIC_lda_exchange_derivative_discontinuity(nEns,wEns,nGrid,weight,rhow,ExDD)
|
||||
|
||||
! Compute the restricted version of the GIC exchange individual energy
|
||||
|
||||
implicit none
|
||||
include 'parameters.h'
|
||||
|
||||
! Input variables
|
||||
|
||||
integer,intent(in) :: nEns
|
||||
double precision,intent(in) :: wEns(nEns)
|
||||
integer,intent(in) :: nGrid
|
||||
double precision,intent(in) :: weight(nGrid)
|
||||
double precision,intent(in) :: rhow(nGrid)
|
||||
|
||||
! Local variables
|
||||
|
||||
integer :: iEns,jEns
|
||||
integer :: iG
|
||||
double precision :: r
|
||||
double precision :: dExdw(nEns)
|
||||
double precision,external :: Kronecker_delta
|
||||
|
||||
double precision :: a,b,c,w
|
||||
double precision :: dCxGICdw
|
||||
|
||||
! Output variables
|
||||
|
||||
double precision,intent(out) :: ExDD(nEns)
|
||||
|
||||
! Compute correlation energy for ground- and doubly-excited states
|
||||
|
||||
a = + 0.5751782560799208d0
|
||||
b = - 0.021108186591137282d0
|
||||
c = - 0.36718902716347124d0
|
||||
|
||||
w = wEns(2)
|
||||
dCxGICdw = CxLDA*(0.5d0*b + (2d0*a + 0.5d0*c)*(w - 0.5d0) - (1d0 - w)*w*(3d0*b + 4d0*c*(w - 0.5d0)))
|
||||
|
||||
dExdw(:) = 0d0
|
||||
|
||||
do iG=1,nGrid
|
||||
|
||||
r = max(0d0,rhow(iG))
|
||||
|
||||
if(r > threshold) then
|
||||
|
||||
dExdw(1) = 0d0
|
||||
dExdw(2) = dExdw(2) + weight(iG)*dCxGICdw*r**(4d0/3d0)
|
||||
|
||||
end if
|
||||
|
||||
end do
|
||||
|
||||
ExDD(:) = 0d0
|
||||
|
||||
do iEns=1,nEns
|
||||
do jEns=2,nEns
|
||||
|
||||
ExDD(iEns) = ExDD(iEns) + (Kronecker_delta(iEns,jEns) - wEns(jEns))*dExdw(jEns)
|
||||
|
||||
end do
|
||||
end do
|
||||
|
||||
end subroutine RGIC_lda_exchange_derivative_discontinuity
|
52
src/eDFT/RGIC_lda_exchange_energy.f90
Normal file
52
src/eDFT/RGIC_lda_exchange_energy.f90
Normal file
@ -0,0 +1,52 @@
|
||||
subroutine RGIC_lda_exchange_energy(nEns,wEns,nGrid,weight,rho,Ex)
|
||||
|
||||
! Compute the restricted version of the GIC exchange functional
|
||||
|
||||
implicit none
|
||||
include 'parameters.h'
|
||||
|
||||
! Input variables
|
||||
|
||||
integer,intent(in) :: nEns
|
||||
double precision,intent(in) :: wEns(nEns)
|
||||
integer,intent(in) :: nGrid
|
||||
double precision,intent(in) :: weight(nGrid)
|
||||
double precision,intent(in) :: rho(nGrid)
|
||||
|
||||
! Local variables
|
||||
|
||||
integer :: iG
|
||||
double precision :: r
|
||||
|
||||
double precision :: a,b,c,w
|
||||
double precision :: CxGIC
|
||||
|
||||
! Output variables
|
||||
|
||||
double precision :: Ex
|
||||
|
||||
! Weight-denepdent Cx coefficient
|
||||
|
||||
a = + 0.5751782560799208d0
|
||||
b = - 0.021108186591137282d0
|
||||
c = - 0.36718902716347124d0
|
||||
|
||||
w = wEns(2)
|
||||
CxGIC = CxLDA*w*(1d0 - w)*(a + b*(w - 0.5d0) + c*(w - 0.5d0)**2)
|
||||
|
||||
! Compute GIC-LDA exchange energy
|
||||
|
||||
Ex = 0d0
|
||||
|
||||
do iG=1,nGrid
|
||||
|
||||
r = max(0d0,rho(iG))
|
||||
|
||||
if(r > threshold) then
|
||||
Ex = Ex + weight(iG)*CxLDA*r**(4d0/3d0)
|
||||
Ex = Ex + weight(iG)*CxGIC*r**(4d0/3d0)
|
||||
endif
|
||||
|
||||
enddo
|
||||
|
||||
end subroutine RGIC_lda_exchange_energy
|
61
src/eDFT/RGIC_lda_exchange_individual_energy.f90
Normal file
61
src/eDFT/RGIC_lda_exchange_individual_energy.f90
Normal file
@ -0,0 +1,61 @@
|
||||
subroutine RGIC_lda_exchange_individual_energy(nEns,wEns,nGrid,weight,rhow,rho,Ex)
|
||||
|
||||
! Compute the restricted version of the GIC exchange functional
|
||||
|
||||
implicit none
|
||||
include 'parameters.h'
|
||||
|
||||
! Input variables
|
||||
|
||||
integer,intent(in) :: nEns
|
||||
double precision,intent(in) :: wEns(nEns)
|
||||
integer,intent(in) :: nGrid
|
||||
double precision,intent(in) :: weight(nGrid)
|
||||
double precision,intent(in) :: rhow(nGrid)
|
||||
double precision,intent(in) :: rho(nGrid)
|
||||
|
||||
! Local variables
|
||||
|
||||
integer :: iG
|
||||
double precision :: CxGIC
|
||||
double precision :: r,rI
|
||||
double precision :: e_p,dedr
|
||||
|
||||
double precision :: a,b,c,w
|
||||
|
||||
! Output variables
|
||||
|
||||
double precision,intent(out) :: Ex
|
||||
|
||||
! Weight-dependent Cx coefficient for RMFL20 exchange functional
|
||||
|
||||
a = + 0.5751782560799208d0
|
||||
b = - 0.021108186591137282d0
|
||||
c = - 0.36718902716347124d0
|
||||
|
||||
w = wEns(2)
|
||||
CxGIC = CxLDA*w*(1d0 - w)*(a + b*(w - 0.5d0) + c*(w - 0.5d0)**2)
|
||||
|
||||
! Compute LDA exchange matrix in the AO basis
|
||||
|
||||
Ex = 0d0
|
||||
do iG=1,nGrid
|
||||
|
||||
r = max(0d0,rhow(iG))
|
||||
rI = max(0d0,rho(iG))
|
||||
|
||||
if(r > threshold .and. rI > threshold) then
|
||||
|
||||
e_p = CxLDA*r**(1d0/3d0)
|
||||
dedr = 1d0/3d0*CxLDA*r**(-2d0/3d0)
|
||||
Ex = Ex + weight(iG)*(e_p*rI + dedr*r*rI - dedr*r*r)
|
||||
|
||||
e_p = CxGIC*r**(1d0/3d0)
|
||||
dedr = 1d0/3d0*CxGIC*r**(-2d0/3d0)
|
||||
Ex = Ex + weight(iG)*(e_p*rI + dedr*r*rI - dedr*r*r)
|
||||
|
||||
endif
|
||||
|
||||
enddo
|
||||
|
||||
end subroutine RGIC_lda_exchange_individual_energy
|
61
src/eDFT/RGIC_lda_exchange_potential.f90
Normal file
61
src/eDFT/RGIC_lda_exchange_potential.f90
Normal file
@ -0,0 +1,61 @@
|
||||
subroutine RGIC_lda_exchange_potential(nEns,wEns,nGrid,weight,nBas,AO,rho,Fx)
|
||||
|
||||
! Compute the restricted version of the GIC exchange potential
|
||||
|
||||
implicit none
|
||||
include 'parameters.h'
|
||||
|
||||
! Input variables
|
||||
|
||||
integer,intent(in) :: nEns
|
||||
double precision,intent(in) :: wEns(nEns)
|
||||
integer,intent(in) :: nGrid
|
||||
double precision,intent(in) :: weight(nGrid)
|
||||
integer,intent(in) :: nBas
|
||||
double precision,intent(in) :: AO(nBas,nGrid)
|
||||
double precision,intent(in) :: rho(nGrid)
|
||||
|
||||
! Local variables
|
||||
|
||||
integer :: mu,nu,iG
|
||||
double precision :: r,vAO
|
||||
|
||||
double precision :: a,b,c,w
|
||||
double precision :: CxGIC
|
||||
|
||||
! Output variables
|
||||
|
||||
double precision,intent(out) :: Fx(nBas,nBas)
|
||||
|
||||
! Weight-dependent Cx coefficient for RMFL20 exchange functional
|
||||
|
||||
a = + 0.5751782560799208d0
|
||||
b = - 0.021108186591137282d0
|
||||
c = - 0.36718902716347124d0
|
||||
|
||||
w = wEns(2)
|
||||
CxGIC = CxLDA*w*(1d0 - w)*(a + b*(w - 0.5d0) + c*(w - 0.5d0)**2)
|
||||
|
||||
! Compute LDA exchange matrix in the AO basis
|
||||
|
||||
Fx(:,:) = 0d0
|
||||
|
||||
do mu=1,nBas
|
||||
do nu=1,nBas
|
||||
do iG=1,nGrid
|
||||
|
||||
r = max(0d0,rho(iG))
|
||||
|
||||
if(r > threshold) then
|
||||
|
||||
vAO = weight(iG)*AO(mu,iG)*AO(nu,iG)
|
||||
Fx(mu,nu) = Fx(mu,nu) + vAO*4d0/3d0*CxLDA*r**(1d0/3d0)
|
||||
Fx(mu,nu) = Fx(mu,nu) + vAO*4d0/3d0*CxGIC*r**(1d0/3d0)
|
||||
|
||||
endif
|
||||
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
|
||||
end subroutine RGIC_lda_exchange_potential
|
@ -34,8 +34,10 @@ subroutine RMFL20_lda_exchange_derivative_discontinuity(nEns,wEns,nGrid,weight,r
|
||||
r = max(0d0,rhow(iG))
|
||||
|
||||
if(r > threshold) then
|
||||
dExdw(1) = dExdw(1) + weight(iG)*Cx0*r**(4d0/3d0)
|
||||
dExdw(2) = dExdw(2) + weight(iG)*Cx1*r**(4d0/3d0)
|
||||
|
||||
dExdw(1) = 0d0
|
||||
dExdw(2) = dExdw(2) + weight(iG)*(Cx1 - Cx0)*r**(4d0/3d0)
|
||||
|
||||
end if
|
||||
|
||||
end do
|
||||
@ -43,9 +45,9 @@ subroutine RMFL20_lda_exchange_derivative_discontinuity(nEns,wEns,nGrid,weight,r
|
||||
ExDD(:) = 0d0
|
||||
|
||||
do iEns=1,nEns
|
||||
do jEns=1,nEns
|
||||
do jEns=2,nEns
|
||||
|
||||
ExDD(iEns) = ExDD(iEns) + (Kronecker_delta(iEns,jEns) - wEns(jEns))*(dExdw(jEns) - dExdw(1))
|
||||
ExDD(iEns) = ExDD(iEns) + (Kronecker_delta(iEns,jEns) - wEns(jEns))*dExdw(jEns)
|
||||
|
||||
end do
|
||||
end do
|
||||
|
@ -20,7 +20,7 @@ subroutine RMFL20_lda_exchange_individual_energy(LDA_centered,nEns,wEns,nGrid,we
|
||||
integer :: iG
|
||||
double precision :: Cxw
|
||||
double precision :: r,rI
|
||||
double precision :: e,dedr
|
||||
double precision :: e_p,dedr
|
||||
|
||||
! Output variables
|
||||
|
||||
@ -44,9 +44,9 @@ subroutine RMFL20_lda_exchange_individual_energy(LDA_centered,nEns,wEns,nGrid,we
|
||||
|
||||
if(r > threshold .and. rI > threshold) then
|
||||
|
||||
e = Cxw*r**(1d0/3d0)
|
||||
e_p = Cxw*r**(1d0/3d0)
|
||||
dedr = 1d0/3d0*Cxw*r**(-2d0/3d0)
|
||||
Ex = Ex + weight(iG)*(e*rI + dedr*r*rI - dedr*r*r)
|
||||
Ex = Ex + weight(iG)*(e_p*rI + dedr*r*rI - dedr*r*r)
|
||||
|
||||
endif
|
||||
|
||||
|
@ -24,8 +24,8 @@ subroutine fock_exchange_individual_energy(nBas,Pw,P,ERI,Ex)
|
||||
|
||||
allocate(Fx(nBas,nBas))
|
||||
|
||||
call fock_exchange_potential(nBas,P(:,:),ERI(:,:,:,:),Fx(:,:))
|
||||
|
||||
Ex = 0.5d0*trace_matrix(nBas,matmul(P(:,:),Fx(:,:))) !&
|
||||
call fock_exchange_potential(nBas,Pw(:,:),ERI(:,:,:,:),Fx(:,:))
|
||||
Ex = trace_matrix(nBas,matmul(P(:,:),Fx(:,:))) &
|
||||
- 0.5d0*trace_matrix(nBas,matmul(Pw(:,:),Fx(:,:)))
|
||||
|
||||
end subroutine fock_exchange_individual_energy
|
||||
|
@ -28,8 +28,9 @@ subroutine hartree_individual_energy(rung,nBas,ERI,J,Pw,P,EJ)
|
||||
|
||||
case(0)
|
||||
|
||||
call hartree_coulomb(nBas,P(:,:),ERI(:,:,:,:),J(:,:))
|
||||
EJ = 0.5d0*trace_matrix(nBas,matmul(P(:,:),J(:,:)))
|
||||
call hartree_coulomb(nBas,Pw(:,:),ERI(:,:,:,:),J(:,:))
|
||||
EJ = trace_matrix(nBas,matmul(P(:,:),J(:,:))) &
|
||||
- 0.5d0*trace_matrix(nBas,matmul(Pw(:,:),J(:,:)))
|
||||
|
||||
! LDA functionals
|
||||
|
||||
@ -57,8 +58,9 @@ subroutine hartree_individual_energy(rung,nBas,ERI,J,Pw,P,EJ)
|
||||
|
||||
case(666)
|
||||
|
||||
call hartree_coulomb(nBas,P(:,:),ERI(:,:,:,:),J(:,:))
|
||||
EJ = 0.5d0*trace_matrix(nBas,matmul(P(:,:),J(:,:)))
|
||||
call hartree_coulomb(nBas,Pw(:,:),ERI(:,:,:,:),J(:,:))
|
||||
EJ = trace_matrix(nBas,matmul(P(:,:),J(:,:))) &
|
||||
- 0.5d0*trace_matrix(nBas,matmul(Pw(:,:),J(:,:)))
|
||||
|
||||
end select
|
||||
|
||||
|
@ -37,6 +37,10 @@ subroutine lda_exchange_derivative_discontinuity(DFA,nEns,wEns,nGrid,weight,rhow
|
||||
|
||||
call RMFL20_lda_exchange_derivative_discontinuity(nEns,wEns,nGrid,weight(:),rhow(:),ExDD(:))
|
||||
|
||||
case ('RGIC')
|
||||
|
||||
call RGIC_lda_exchange_derivative_discontinuity(nEns,wEns,nGrid,weight(:),rhow(:),ExDD(:))
|
||||
|
||||
case default
|
||||
|
||||
call print_warning('!!! LDA exchange functional not available !!!')
|
||||
|
@ -23,24 +23,22 @@ subroutine lda_exchange_energy(DFA,LDA_centered,nEns,wEns,nGrid,weight,rho,Ex)
|
||||
|
||||
select case (DFA)
|
||||
|
||||
! Slater's LDA correlation functional
|
||||
|
||||
case ('S51')
|
||||
|
||||
call S51_lda_exchange_energy(nGrid,weight,rho,Ex)
|
||||
|
||||
! Restricted version of Slater's LDA correlation functional
|
||||
|
||||
case ('RS51')
|
||||
|
||||
call RS51_lda_exchange_energy(nGrid,weight,rho,Ex)
|
||||
|
||||
! Restricted version of the weight-dependent Marut-Fromager-Loos 2020 exchange functional
|
||||
|
||||
case ('RMFL20')
|
||||
|
||||
call RMFL20_lda_exchange_energy(LDA_centered,nEns,wEns,nGrid,weight,rho,Ex)
|
||||
|
||||
case ('RGIC')
|
||||
|
||||
call RGIC_lda_exchange_energy(nEns,wEns,nGrid,weight,rho,Ex)
|
||||
|
||||
case default
|
||||
|
||||
call print_warning('!!! LDA exchange functional not available !!!')
|
||||
|
@ -32,6 +32,10 @@ subroutine lda_exchange_individual_energy(DFA,LDA_centered,nEns,wEns,nGrid,weigh
|
||||
|
||||
call RMFL20_lda_exchange_individual_energy(LDA_centered,nEns,wEns,nGrid,weight(:),rhow(:),rho(:),Ex)
|
||||
|
||||
case ('RGIC')
|
||||
|
||||
call RGIC_lda_exchange_individual_energy(nEns,wEns,nGrid,weight(:),rhow(:),rho(:),Ex)
|
||||
|
||||
case default
|
||||
|
||||
call print_warning('!!! LDA correlation functional not available !!!')
|
||||
|
@ -26,24 +26,22 @@ subroutine lda_exchange_potential(DFA,LDA_centered,nEns,wEns,nGrid,weight,nBas,A
|
||||
|
||||
select case (DFA)
|
||||
|
||||
! Restricted version of Slater's LDA correlation functional
|
||||
|
||||
case ('RS51')
|
||||
|
||||
call RS51_lda_exchange_potential(nGrid,weight,nBas,AO,rho,Fx)
|
||||
|
||||
! Slater's LDA correlation functional
|
||||
|
||||
case ('S51')
|
||||
|
||||
call S51_lda_exchange_potential(nGrid,weight,nBas,AO,rho,Fx)
|
||||
|
||||
! Restricted version of the weight-dependent Marut-Fromager-Loos 2020 functional
|
||||
|
||||
case ('RMFL20')
|
||||
|
||||
call RMFL20_lda_exchange_potential(LDA_centered,nEns,wEns,nGrid,weight,nBas,AO,rho,Fx)
|
||||
|
||||
case ('RGIC')
|
||||
|
||||
call RGIC_lda_exchange_potential(nEns,wEns,nGrid,weight,nBas,AO,rho,Fx)
|
||||
|
||||
case default
|
||||
|
||||
call print_warning('!!! LDA exchange functional not available !!!')
|
||||
|
Loading…
Reference in New Issue
Block a user