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mirror of https://github.com/pfloos/quack synced 2024-06-02 03:15:33 +02:00
QuAcK/src/QuAcK/BSE2_A_matrix_dynamic.f90
2020-06-04 13:08:31 +02:00

169 lines
5.1 KiB
Fortran

subroutine BSE2_A_matrix_dynamic(ispin,eta,nBas,nC,nO,nV,nR,nS,lambda,ERI,eGF,OmBSE,A_dyn,ZA_dyn)
! Compute the resonant part of the dynamic BSE2 matrix
implicit none
include 'parameters.h'
! Input variables
integer,intent(in) :: ispin
integer,intent(in) :: nBas,nC,nO,nV,nR,nS
double precision,intent(in) :: eta
double precision,intent(in) :: lambda
double precision,intent(in) :: ERI(nBas,nBas,nBas,nBas)
double precision,intent(in) :: eGF(nBas)
double precision,intent(in) :: OmBSE
! Local variables
double precision :: dem,num
integer :: i,j,k,l
integer :: a,b,c,d
integer :: ia,jb
! Output variables
double precision,intent(out) :: A_dyn(nS,nS)
double precision,intent(out) :: ZA_dyn(nS,nS)
! Initialization
A_dyn(:,:) = 0d0
ZA_dyn(:,:) = 0d0
! Second-order correlation kernel for the block A of the singlet manifold
if(ispin == 1) then
ia = 0
do i=nC+1,nO
do a=nO+1,nBas-nR
ia = ia + 1
jb = 0
do j=nC+1,nO
do b=nO+1,nBas-nR
jb = jb + 1
do k=nC+1,nO
do c=nO+1,nBas-nR
dem = OmBSE - eGF(a) + eGF(k) - eGF(c) + eGF(j)
num = 2d0*ERI(j,k,i,c)*ERI(a,c,b,k) - ERI(j,k,i,c)*ERI(a,c,k,b) &
- ERI(j,k,c,i)*ERI(a,c,b,k) + 2d0*ERI(j,k,c,i)*ERI(a,c,k,b)
A_dyn(ia,jb) = A_dyn(ia,jb) - num*dem/(dem**2 + eta**2)
ZA_dyn(ia,jb) = ZA_dyn(ia,jb) + num*(dem**2 - eta**2)/(dem**2 + eta**2)**2
dem = OmBSE + eGF(i) - eGF(c) + eGF(k) - eGF(b)
num = 2d0*ERI(j,c,i,k)*ERI(a,k,b,c) - ERI(j,c,i,k)*ERI(a,k,c,b) &
- ERI(j,c,k,i)*ERI(a,k,b,c) + 2d0*ERI(j,c,k,i)*ERI(a,k,c,b)
A_dyn(ia,jb) = A_dyn(ia,jb) - num*dem/(dem**2 + eta**2)
ZA_dyn(ia,jb) = ZA_dyn(ia,jb) + num*(dem**2 - eta**2)/(dem**2 + eta**2)**2
end do
end do
do c=nO+1,nBas-nR
do d=nO+1,nBas-nR
dem = OmBSE + eGF(i) + eGF(j) - eGF(c) - eGF(d)
num = 2d0*ERI(a,j,c,d)*ERI(c,d,i,b) - ERI(a,j,c,d)*ERI(c,d,b,i) &
- ERI(a,j,d,c)*ERI(c,d,i,b) + 2d0*ERI(a,j,d,c)*ERI(c,d,b,i)
A_dyn(ia,jb) = A_dyn(ia,jb) + 0.5d0*num*dem/(dem**2 + eta**2)
ZA_dyn(ia,jb) = ZA_dyn(ia,jb) - 0.5d0*num*(dem**2 - eta**2)/(dem**2 + eta**2)**2
end do
end do
do k=nC+1,nO
do l=nC+1,nO
dem = OmBSE - eGF(a) - eGF(b) + eGF(k) + eGF(l)
num = 2d0*ERI(a,j,k,l)*ERI(k,l,i,b) - ERI(a,j,k,l)*ERI(k,l,b,i) &
- ERI(a,j,l,k)*ERI(k,l,i,b) + 2d0*ERI(a,j,l,k)*ERI(k,l,b,i)
A_dyn(ia,jb) = A_dyn(ia,jb) + 0.5d0*num*dem/(dem**2 + eta**2)
ZA_dyn(ia,jb) = ZA_dyn(ia,jb) - 0.5d0*num*(dem**2 - eta**2)/(dem**2 + eta**2)**2
end do
end do
end do
end do
end do
end do
end if
! Second-order correlation kernel for the block A of the triplet manifold
if(ispin == 2) then
ia = 0
do i=nC+1,nO
do a=nO+1,nBas-nR
ia = ia + 1
jb = 0
do j=nC+1,nO
do b=nO+1,nBas-nR
jb = jb + 1
do k=nC+1,nO
do c=nO+1,nBas-nR
dem = OmBSE - eGF(a) + eGF(k) - eGF(c) + eGF(j)
num = 2d0*ERI(j,k,i,c)*ERI(a,c,b,k) - ERI(j,k,i,c)*ERI(a,c,k,b) - ERI(j,k,c,i)*ERI(a,c,b,k)
A_dyn(ia,jb) = A_dyn(ia,jb) - num*dem/(dem**2 + eta**2)
ZA_dyn(ia,jb) = ZA_dyn(ia,jb) + num*(dem**2 - eta**2)/(dem**2 + eta**2)**2
dem = OmBSE + eGF(i) - eGF(c) + eGF(k) - eGF(b)
num = 2d0*ERI(j,c,i,k)*ERI(a,k,b,c) - ERI(j,c,i,k)*ERI(a,k,c,b) - ERI(j,c,k,i)*ERI(a,k,b,c)
A_dyn(ia,jb) = A_dyn(ia,jb) - num*dem/(dem**2 + eta**2)
ZA_dyn(ia,jb) = ZA_dyn(ia,jb) + num*(dem**2 - eta**2)/(dem**2 + eta**2)**2
end do
end do
do c=nO+1,nBas-nR
do d=nO+1,nBas-nR
dem = OmBSE + eGF(i) + eGF(j) - eGF(c) - eGF(d)
num = ERI(a,j,c,d)*ERI(c,d,b,i) + ERI(a,j,d,c)*ERI(c,d,i,b)
A_dyn(ia,jb) = A_dyn(ia,jb) - 0.5d0*num*dem/(dem**2 + eta**2)
ZA_dyn(ia,jb) = ZA_dyn(ia,jb) + 0.5d0*num*(dem**2 - eta**2)/(dem**2 + eta**2)**2
end do
end do
do k=nC+1,nO
do l=nC+1,nO
dem = OmBSE - eGF(a) - eGF(b) + eGF(k) + eGF(l)
num = ERI(a,j,k,l)*ERI(k,l,b,i) + ERI(a,j,l,k)*ERI(k,l,i,b)
A_dyn(ia,jb) = A_dyn(ia,jb) - 0.5d0*num*dem/(dem**2 + eta**2)
ZA_dyn(ia,jb) = ZA_dyn(ia,jb) + 0.5d0*num*(dem**2 - eta**2)/(dem**2 + eta**2)**2
end do
end do
end do
end do
end do
end do
end if
end subroutine BSE2_A_matrix_dynamic