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https://github.com/pfloos/quack
synced 2024-11-19 04:22:39 +01:00
root search for GTeh
This commit is contained in:
parent
866ed94153
commit
044058ac66
@ -11,9 +11,9 @@
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# phRPA* phRPAx* crRPA ppRPA
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F F F F
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# G0F2* evGF2* qsGF2* G0F3 evGF3
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T F F F F
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F F F F F
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# G0W0* evGW* qsGW* SRG-qsGW ufG0W0 ufGW
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F F F F F F
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# G0T0pp evGTpp qsGTpp G0T0eh evGTeh qsGTeh
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F F F F F F
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F F F T F F
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# * unrestricted version available
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@ -9,10 +9,10 @@
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# GF: maxSCF thresh DIIS n_diis lin eta renorm reg
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256 0.00001 T 5 T 0.0 0 F
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# GW: maxSCF thresh DIIS n_diis lin eta TDA_W reg
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256 0.00001 T 5 T 0.0 F F
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256 0.00001 T 5 F 0.0 F F
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# GT: maxSCF thresh DIIS n_diis lin eta TDA_T reg
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256 0.00001 T 5 T 0.0 F F
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256 0.00001 T 5 F 0.0 F F
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# ACFDT: AC Kx XBS
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F F T
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# BSE: phBSE phBSE2 ppBSE dBSE dTDA
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F F T T T
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F F F F T
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@ -155,9 +155,11 @@ subroutine G0T0eh(doACFDT,exchange_kernel,doXBS,dophBSE,dophBSE2,TDA_T,TDA,dBSE,
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else
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write(*,*) ' *** Root search not yet implemented in G0T0eh *** '
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write(*,*) ' *** Quasiparticle energies obtained by root search (experimental) *** '
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write(*,*)
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call GTeh_QP_graph(eta,nBas,nC,nO,nV,nR,nS,eHF,Om,rhoL,rhoR,eGTlin,eGT)
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end if
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! Compute the RPA correlation energy based on the G0T0eh quasiparticle energies
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@ -192,7 +192,7 @@ subroutine G0T0pp(doACFDT,exchange_kernel,doXBS,dophBSE,TDA_T,TDA,dBSE,dTDA,dopp
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write(*,*) ' *** Quasiparticle energies obtained by root search (experimental) *** '
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write(*,*)
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call QP_graph_GT(eta,nBas,nC,nO,nV,nR,nOOaa,nVVaa,eHF,Om1aa,rho1aa,Om2aa,rho2aa,eGTlin,eGT)
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call GTpp_QP_graph(eta,nBas,nC,nO,nV,nR,nOOaa,nVVaa,eHF,Om1aa,rho1aa,Om2aa,rho2aa,eGTlin,eGT)
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end if
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75
src/GT/GTeh_QP_graph.f90
Normal file
75
src/GT/GTeh_QP_graph.f90
Normal file
@ -0,0 +1,75 @@
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subroutine GTeh_QP_graph(eta,nBas,nC,nO,nV,nR,nS,eHF,Om,rhoL,rhoR,eGTlin,eGT)
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implicit none
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include 'parameters.h'
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! Iput variables
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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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integer,intent(in) :: nS
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double precision,intent(in) :: eta
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double precision,intent(in) :: eHF(nBas)
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double precision,intent(in) :: Om(nS)
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double precision,intent(in) :: rhoL(nBas,nBas,nS,2)
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double precision,intent(in) :: rhoR(nBas,nBas,nS,2)
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double precision,intent(in) :: eGTlin(nBas)
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! Local variables
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integer :: p
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integer :: nIt
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integer,parameter :: maxIt = 64
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double precision,parameter :: thresh = 1d-6
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double precision,external :: GTeh_SigC,GTeh_dSigC
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double precision :: sigC,dsigC
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double precision :: f,df
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double precision :: w
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! Output variables
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double precision,intent(out) :: eGT(nBas)
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sigC = 0d0
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dsigC = 0d0
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! Run Newton's algorithm to find the root
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do p=nC+1,nBas-nR
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write(*,*) '-----------------'
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write(*,'(A10,I3)') 'Orbital ',p
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write(*,*) '-----------------'
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w = eGTlin(p)
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nIt = 0
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f = 1d0
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write(*,'(A3,I3,A1,1X,3F15.9)') 'It.',nIt,':',w*HaToeV,f
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do while (abs(f) > thresh .and. nIt < maxIt)
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nIt = nIt + 1
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sigC = GTeh_SigC(p,w,eta,nBas,nC,nO,nV,nR,nS,eHF,Om,rhoL,rhoR)
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dsigC = GTeh_dSigC(p,w,eta,nBas,nC,nO,nV,nR,nS,eHF,Om,rhoL,rhoR)
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f = w - eHF(p) - sigC
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df = 1d0 - dsigC
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w = w - f/df
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write(*,'(A3,I3,A1,1X,3F15.9)') 'It.',nIt,':',w*HaToeV,f,sigC
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end do
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if(nIt == maxIt) then
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write(*,*) 'Newton root search has not converged!'
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else
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eGT(p) = w
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write(*,'(A32,F16.10)') 'Quasiparticle energy (eV) ',eGT(p)*HaToeV
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write(*,*)
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end if
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end do
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end subroutine
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53
src/GT/GTeh_SigC.f90
Normal file
53
src/GT/GTeh_SigC.f90
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@ -0,0 +1,53 @@
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double precision function GTeh_SigC(p,w,eta,nBas,nC,nO,nV,nR,nS,e,Om,rhoL,rhoR)
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! Compute diagonal of the correlation part of the self-energy
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implicit none
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include 'parameters.h'
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! Input variables
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integer,intent(in) :: p
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double precision,intent(in) :: w
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double precision,intent(in) :: eta
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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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integer,intent(in) :: nS
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double precision,intent(in) :: e(nBas)
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double precision,intent(in) :: Om(nS)
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double precision,intent(in) :: rhoL(nBas,nBas,nS,2)
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double precision,intent(in) :: rhoR(nBas,nBas,nS,2)
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! Local variables
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integer :: i,a,m
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double precision :: num,eps
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! Initialize
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GTeh_SigC = 0d0
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! Occupied part of the correlation self-energy
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do i=nC+1,nO
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do m=1,nS
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eps = w - e(i) + Om(m)
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num = rhoL(i,p,m,1)*rhoR(i,p,m,2)
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GTeh_SigC = GTeh_SigC + num*eps/(eps**2 + eta**2)
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enddo
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enddo
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! Virtual part of the correlation self-energy
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do a=nO+1,nBas-nR
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do m=1,nS
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eps = w - e(a) - Om(m)
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num = rhoL(p,a,m,1)*rhoR(p,a,m,2)
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GTeh_SigC = GTeh_SigC + num*eps/(eps**2 + eta**2)
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enddo
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enddo
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end function
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53
src/GT/GTeh_dSigC.f90
Normal file
53
src/GT/GTeh_dSigC.f90
Normal file
@ -0,0 +1,53 @@
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double precision function GTeh_dSigC(p,w,eta,nBas,nC,nO,nV,nR,nS,e,Om,rhoL,rhoR)
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! Compute the derivative of the correlation part of the self-energy
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implicit none
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include 'parameters.h'
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! Input variables
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integer,intent(in) :: p
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double precision,intent(in) :: w
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double precision,intent(in) :: eta
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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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integer,intent(in) :: nS
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double precision,intent(in) :: e(nBas)
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double precision,intent(in) :: Om(nS)
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double precision,intent(in) :: rhoL(nBas,nBas,nS,2)
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double precision,intent(in) :: rhoR(nBas,nBas,nS,2)
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! Local variables
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integer :: i,a,m
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double precision :: num,eps
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! Initialize
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GTeh_dSigC = 0d0
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! Occupied part of the correlation self-energy
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do i=nC+1,nO
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do m=1,nS
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eps = w - e(i) + Om(m)
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num = rhoL(i,p,m,1)*rhoR(i,p,m,2)
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GTeh_dSigC = GTeh_dSigC - num*(eps**2 - eta**2)/(eps**2 + eta**2)**2
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enddo
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enddo
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! Virtual part of the correlation self-energy
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do a=nO+1,nBas-nR
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do m=1,nS
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eps = w - e(a) - Om(m)
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num = rhoL(p,a,m,1)*rhoR(p,a,m,2)
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GTeh_dSigC = GTeh_dSigC - num*(eps**2 - eta**2)/(eps**2 + eta**2)**2
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enddo
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enddo
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end function
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@ -51,12 +51,12 @@ subroutine GTeh_excitation_density(nBas,nC,nO,nR,nS,ERI,XpY,XmY,rhoL,rhoR)
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do m=1,nS
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rhoL(p,q,m,1) = rhoL(p,q,m,1) + ERI(p,j,b,q)*X(jb,m) + ERI(p,b,j,q)*Y(jb,m)
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rhoL(p,q,m,2) = rhoL(p,q,m,2) + ERI(b,p,q,j)*Y(jb,m) + ERI(j,p,q,b)*X(jb,m)
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rhoL(p,q,m,2) = rhoL(p,q,m,2) + ERI(p,j,b,q)*Y(jb,m) + ERI(p,b,j,q)*X(jb,m)
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rhoR(p,q,m,1) = rhoR(p,q,m,1) &
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+ (2d0*ERI(b,q,p,j) - ERI(b,q,j,p))*X(jb,m) + (2d0*ERI(j,q,p,b) - ERI(j,q,b,p))*Y(jb,m)
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+ (2d0*ERI(p,j,b,q) - ERI(p,j,q,b))*X(jb,m) + (2d0*ERI(p,b,j,q) - ERI(p,b,q,j))*Y(jb,m)
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rhoR(p,q,m,2) = rhoR(p,q,m,2) &
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+ (2d0*ERI(b,p,q,j) - ERI(b,p,j,q))*Y(jb,m) + (2d0*ERI(j,p,q,b) - ERI(j,p,b,q))*X(jb,m)
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+ (2d0*ERI(p,j,b,q) - ERI(p,j,q,b))*Y(jb,m) + (2d0*ERI(p,b,j,q) - ERI(p,b,q,j))*X(jb,m)
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enddo
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enddo
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@ -46,7 +46,7 @@ subroutine GTeh_self_energy_diag(eta,nBas,nC,nO,nV,nR,nS,e,Om,rhoL,rhoR,EcGM,Sig
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do m=1,nS
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eps = e(p) - e(i) + Om(m)
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num = rhoL(p,i,m,2)*rhoR(i,p,m,2)
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num = rhoL(i,p,m,1)*rhoR(i,p,m,2)
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Sig(p) = Sig(p) + num*eps/(eps**2 + eta**2)
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Z(p) = Z(p) - num*(eps**2 - eta**2)/(eps**2 + eta**2)**2
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@ -61,7 +61,7 @@ subroutine GTeh_self_energy_diag(eta,nBas,nC,nO,nV,nR,nS,e,Om,rhoL,rhoR,EcGM,Sig
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do m=1,nS
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eps = e(p) - e(a) - Om(m)
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num = rhoL(a,p,m,1)*rhoR(p,a,m,1)
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num = rhoL(p,a,m,1)*rhoR(p,a,m,2)
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Sig(p) = Sig(p) + num*eps/(eps**2 + eta**2)
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Z(p) = Z(p) - num*(eps**2 - eta**2)/(eps**2 + eta**2)**2
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@ -1,4 +1,4 @@
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subroutine QP_graph_GT(eta,nBas,nC,nO,nV,nR,nOO,nVV,eHF,Omega1,rho1,Omega2,rho2,eGTlin,eGT)
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subroutine GTpp_QP_graph(eta,nBas,nC,nO,nV,nR,nOO,nVV,eHF,Om1,rho1,Om2,rho2,eGTlin,eGT)
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implicit none
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include 'parameters.h'
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@ -14,9 +14,9 @@ subroutine QP_graph_GT(eta,nBas,nC,nO,nV,nR,nOO,nVV,eHF,Omega1,rho1,Omega2,rho2,
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double precision,intent(in) :: eta
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double precision,intent(in) :: eHF(nBas)
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double precision,intent(in) :: Omega1(nVV)
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double precision,intent(in) :: Om1(nVV)
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double precision,intent(in) :: rho1(nBas,nBas,nVV)
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double precision,intent(in) :: Omega2(nOO)
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double precision,intent(in) :: Om2(nOO)
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double precision,intent(in) :: rho2(nBas,nBas,nOO)
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double precision,intent(in) :: eGTlin(nBas)
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@ -26,7 +26,7 @@ subroutine QP_graph_GT(eta,nBas,nC,nO,nV,nR,nOO,nVV,eHF,Omega1,rho1,Omega2,rho2,
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integer :: nIt
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integer,parameter :: maxIt = 64
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double precision,parameter :: thresh = 1d-6
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double precision,external :: SigmaC_GT,dSigmaC_GT
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double precision,external :: GTpp_SigC,GTpp_dSigC
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double precision :: sigC,dsigC
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double precision :: f,df
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double precision :: w
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@ -54,8 +54,8 @@ subroutine QP_graph_GT(eta,nBas,nC,nO,nV,nR,nOO,nVV,eHF,Omega1,rho1,Omega2,rho2,
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nIt = nIt + 1
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sigC = SigmaC_GT(p,w,eta,nBas,nC,nO,nV,nR,nOO,nVV,eHF,Omega1,rho1,Omega2,rho2)
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dsigC = dSigmaC_GT(p,w,eta,nBas,nC,nO,nV,nR,nOO,nVV,eHF,Omega1,rho1,Omega2,rho2)
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sigC = GTpp_SigC(p,w,eta,nBas,nC,nO,nV,nR,nOO,nVV,eHF,Om1,rho1,Om2,rho2)
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dsigC = GTpp_dSigC(p,w,eta,nBas,nC,nO,nV,nR,nOO,nVV,eHF,Om1,rho1,Om2,rho2)
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write (*,*) sigC
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f = w - eHF(p) - sigC
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df = 1d0 - dsigC
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@ -76,4 +76,4 @@ subroutine QP_graph_GT(eta,nBas,nC,nO,nV,nR,nOO,nVV,eHF,Omega1,rho1,Omega2,rho2,
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end do
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end subroutine QP_graph_GT
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end subroutine
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@ -1,4 +1,4 @@
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double precision function SigmaC_GT(p,w,eta,nBas,nC,nO,nV,nR,nOO,nVV,e,Omega1,rho1,Omega2,rho2)
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double precision function GTpp_SigC(p,w,eta,nBas,nC,nO,nV,nR,nOO,nVV,e,Om1,rho1,Om2,rho2)
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! Compute diagonal of the correlation part of the self-energy
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@ -17,9 +17,9 @@ double precision function SigmaC_GT(p,w,eta,nBas,nC,nO,nV,nR,nOO,nVV,e,Omega1,rh
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integer,intent(in) :: nR
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integer,intent(in) :: nOO,nVV
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double precision,intent(in) :: e(nBas)
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double precision,intent(in) :: Omega1(nVV)
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double precision,intent(in) :: Om1(nVV)
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double precision,intent(in) :: rho1(nBas,nBas,nVV)
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double precision,intent(in) :: Omega2(nOO)
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double precision,intent(in) :: Om2(nOO)
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double precision,intent(in) :: rho2(nBas,nBas,nOO)
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! Local variables
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@ -29,7 +29,7 @@ double precision function SigmaC_GT(p,w,eta,nBas,nC,nO,nV,nR,nOO,nVV,e,Omega1,rh
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! Initialize
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SigmaC_GT = 0d0
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GTpp_SigC = 0d0
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!----------------------------------------------
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! Occupied part of the T-matrix self-energy
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@ -37,8 +37,8 @@ double precision function SigmaC_GT(p,w,eta,nBas,nC,nO,nV,nR,nOO,nVV,e,Omega1,rh
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do i=nC+1,nO
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do cd=1,nVV
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eps = w + e(i) - Omega1(cd)
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SigmaC_GT = SigmaC_GT + rho1(p,i,cd)**2*eps/(eps**2 + eta**2)
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eps = w + e(i) - Om1(cd)
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GTpp_SigC = GTpp_SigC + rho1(p,i,cd)**2*eps/(eps**2 + eta**2)
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enddo
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enddo
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@ -48,8 +48,8 @@ double precision function SigmaC_GT(p,w,eta,nBas,nC,nO,nV,nR,nOO,nVV,e,Omega1,rh
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do a=nO+1,nBas-nR
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do kl=1,nOO
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eps = w + e(a) - Omega2(kl)
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SigmaC_GT = SigmaC_GT + rho2(p,a,kl)**2*eps/(eps**2 + eta**2)
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eps = w + e(a) - Om2(kl)
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GTpp_SigC = GTpp_SigC + rho2(p,a,kl)**2*eps/(eps**2 + eta**2)
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enddo
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enddo
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@ -1,4 +1,4 @@
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double precision function dSigmaC_GT(p,w,eta,nBas,nC,nO,nV,nR,nOO,nVV,e,Omega1,rho1,Omega2,rho2)
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double precision function GTpp_dSigC(p,w,eta,nBas,nC,nO,nV,nR,nOO,nVV,e,Om1,rho1,Om2,rho2)
|
||||
|
||||
! Compute diagonal of the correlation part of the self-energy
|
||||
|
||||
@ -18,9 +18,9 @@ double precision function dSigmaC_GT(p,w,eta,nBas,nC,nO,nV,nR,nOO,nVV,e,Omega1,r
|
||||
integer,intent(in) :: nOO
|
||||
integer,intent(in) :: nVV
|
||||
double precision,intent(in) :: e(nBas)
|
||||
double precision,intent(in) :: Omega1(nVV)
|
||||
double precision,intent(in) :: Om1(nVV)
|
||||
double precision,intent(in) :: rho1(nBas,nBas,nVV)
|
||||
double precision,intent(in) :: Omega2(nOO)
|
||||
double precision,intent(in) :: Om2(nOO)
|
||||
double precision,intent(in) :: rho2(nBas,nBas,nOO)
|
||||
|
||||
! Local variables
|
||||
@ -30,7 +30,7 @@ double precision function dSigmaC_GT(p,w,eta,nBas,nC,nO,nV,nR,nOO,nVV,e,Omega1,r
|
||||
|
||||
! Initialize
|
||||
|
||||
dSigmaC_GT = 0d0
|
||||
GTpp_dSigC = 0d0
|
||||
|
||||
!----------------------------------------------
|
||||
! Occupied part of the T-matrix self-energy
|
||||
@ -39,8 +39,8 @@ double precision function dSigmaC_GT(p,w,eta,nBas,nC,nO,nV,nR,nOO,nVV,e,Omega1,r
|
||||
do i=nC+1,nO
|
||||
do cd=1,nVV
|
||||
|
||||
eps = w + e(i) - Omega1(cd)
|
||||
dSigmaC_GT = dSigmaC_GT - rho1(p,i,cd)**2*(eps**2 - eta**2)/(eps**2 + eta**2)**2
|
||||
eps = w + e(i) - Om1(cd)
|
||||
GTpp_dSigC= GTpp_dSigC - rho1(p,i,cd)**2*(eps**2 - eta**2)/(eps**2 + eta**2)**2
|
||||
|
||||
enddo
|
||||
enddo
|
||||
@ -52,8 +52,8 @@ double precision function dSigmaC_GT(p,w,eta,nBas,nC,nO,nV,nR,nOO,nVV,e,Omega1,r
|
||||
|
||||
do a=nO+1,nBas-nR
|
||||
do kl=1,nOO
|
||||
eps = w + e(a) - Omega2(kl)
|
||||
dSigmaC_GT = dSigmaC_GT - rho2(p,a,kl)**2*(eps**2 - eta**2)/(eps**2 + eta**2)**2
|
||||
eps = w + e(a) - Om2(kl)
|
||||
GTpp_dSigC = GTpp_dSigC - rho2(p,a,kl)**2*(eps**2 - eta**2)/(eps**2 + eta**2)**2
|
||||
enddo
|
||||
enddo
|
||||
|
@ -149,7 +149,7 @@ subroutine G0W0(doACFDT,exchange_kernel,doXBS,dophBSE,dophBSE2,TDA_W,TDA,dBSE,dT
|
||||
write(*,*) ' *** Quasiparticle energies obtained by root search (experimental) *** '
|
||||
write(*,*)
|
||||
|
||||
call QP_graph(nBas,nC,nO,nV,nR,nS,eta,eHF,Om,rho,eGWlin,eGW,regularize)
|
||||
call GW_QP_graph(nBas,nC,nO,nV,nR,nS,eta,eHF,Om,rho,eGWlin,eGW,regularize)
|
||||
|
||||
end if
|
||||
|
||||
|
@ -1,4 +1,4 @@
|
||||
subroutine QP_graph(nBas,nC,nO,nV,nR,nS,eta,eHF,Omega,rho,eGWlin,eGW,regularize)
|
||||
subroutine GW_QP_graph(nBas,nC,nO,nV,nR,nS,eta,eHF,Omega,rho,eGWlin,eGW,regularize)
|
||||
|
||||
! Compute the graphical solution of the QP equation
|
||||
|
||||
@ -27,7 +27,7 @@ subroutine QP_graph(nBas,nC,nO,nV,nR,nS,eta,eHF,Omega,rho,eGWlin,eGW,regularize)
|
||||
integer :: nIt
|
||||
integer,parameter :: maxIt = 64
|
||||
double precision,parameter :: thresh = 1d-6
|
||||
double precision,external :: SigmaC,dSigmaC
|
||||
double precision,external :: GW_SigC,GW_dSigC
|
||||
double precision :: sigC,dsigC
|
||||
double precision :: f,df
|
||||
double precision :: w
|
||||
@ -53,8 +53,8 @@ subroutine QP_graph(nBas,nC,nO,nV,nR,nS,eta,eHF,Omega,rho,eGWlin,eGW,regularize)
|
||||
|
||||
nIt = nIt + 1
|
||||
|
||||
sigC = SigmaC(p,w,eta,nBas,nC,nO,nV,nR,nS,eHF,Omega,rho,regularize)
|
||||
dsigC = dSigmaC(p,w,eta,nBas,nC,nO,nV,nR,nS,eHF,Omega,rho,regularize)
|
||||
sigC = GW_SigC(p,w,eta,nBas,nC,nO,nV,nR,nS,eHF,Omega,rho,regularize)
|
||||
dsigC = GW_dSigC(p,w,eta,nBas,nC,nO,nV,nR,nS,eHF,Omega,rho,regularize)
|
||||
f = w - eHF(p) - SigC
|
||||
df = 1d0 - dsigC
|
||||
|
||||
@ -80,4 +80,4 @@ subroutine QP_graph(nBas,nC,nO,nV,nR,nS,eta,eHF,Omega,rho,eGWlin,eGW,regularize)
|
||||
|
||||
end do
|
||||
|
||||
end subroutine QP_graph
|
||||
end subroutine
|
@ -1,4 +1,4 @@
|
||||
double precision function SigmaC(p,w,eta,nBas,nC,nO,nV,nR,nS,e,Omega,rho,regularize)
|
||||
double precision function GW_SigC(p,w,eta,nBas,nC,nO,nV,nR,nS,e,Om,rho,regularize)
|
||||
|
||||
! Compute diagonal of the correlation part of the self-energy
|
||||
|
||||
@ -17,7 +17,7 @@ double precision function SigmaC(p,w,eta,nBas,nC,nO,nV,nR,nS,e,Omega,rho,regular
|
||||
integer,intent(in) :: nR
|
||||
integer,intent(in) :: nS
|
||||
double precision,intent(in) :: e(nBas)
|
||||
double precision,intent(in) :: Omega(nS)
|
||||
double precision,intent(in) :: Om(nS)
|
||||
double precision,intent(in) :: rho(nBas,nBas,nS)
|
||||
logical,intent(in) :: regularize
|
||||
|
||||
@ -29,37 +29,36 @@ double precision function SigmaC(p,w,eta,nBas,nC,nO,nV,nR,nS,e,Omega,rho,regular
|
||||
|
||||
! Initialize
|
||||
|
||||
SigmaC = 0d0
|
||||
|
||||
GW_SigC = 0d0
|
||||
|
||||
if (regularize) then
|
||||
! Occupied part of the correlation self-energy
|
||||
do i=nC+1,nO
|
||||
do jb=1,nS
|
||||
eps = w - e(i) + Omega(jb)
|
||||
Dpijb = e(p) - e(i) + Omega(jb)
|
||||
SigmaC = SigmaC + 2d0*rho(p,i,jb)**2*(1d0-exp(-2d0*eta*Dpijb*Dpijb))/eps
|
||||
eps = w - e(i) + Om(jb)
|
||||
Dpijb = e(p) - e(i) + Om(jb)
|
||||
GW_SigC = GW_SigC + 2d0*rho(p,i,jb)**2*(1d0-exp(-2d0*eta*Dpijb*Dpijb))/eps
|
||||
enddo
|
||||
enddo
|
||||
! Virtual part of the correlation self-energy
|
||||
do a=nO+1,nBas-nR
|
||||
do jb=1,nS
|
||||
eps = w - e(a) - Omega(jb)
|
||||
Dpajb = e(p) - e(a) - Omega(jb)
|
||||
SigmaC = SigmaC + 2d0*rho(p,a,jb)**2*(1d0-exp(-2d0*eta*Dpajb*Dpajb))/eps
|
||||
eps = w - e(a) - Om(jb)
|
||||
Dpajb = e(p) - e(a) - Om(jb)
|
||||
GW_SigC = GW_SigC + 2d0*rho(p,a,jb)**2*(1d0-exp(-2d0*eta*Dpajb*Dpajb))/eps
|
||||
enddo
|
||||
enddo
|
||||
|
||||
! We add the static SRG term in the self-energy directly
|
||||
! do i=nC+1,nO
|
||||
! do jb=1,nS
|
||||
! Dpijb = e(p) - e(i) + Omega(jb)
|
||||
! Dpijb = e(p) - e(i) + Om(jb)
|
||||
! SigmaC = SigmaC + 2d0*rho(p,i,jb)**2*(exp(-2d0*eta*Dpijb*Dpijb)/Dpijb)
|
||||
! enddo
|
||||
! enddo
|
||||
! do a=nO+1,nBas-nR
|
||||
! do jb=1,nS
|
||||
! Dpajb = e(p) - e(a) - Omega(jb)
|
||||
! Dpajb = e(p) - e(a) - Om(jb)
|
||||
! SigmaC = SigmaC + 2d0*rho(p,a,jb)**2*(exp(-2d0*eta*Dpajb*Dpajb)/Dpajb)
|
||||
! enddo
|
||||
! enddo
|
||||
@ -68,17 +67,17 @@ double precision function SigmaC(p,w,eta,nBas,nC,nO,nV,nR,nS,e,Omega,rho,regular
|
||||
! Occupied part of the correlation self-energy
|
||||
do i=nC+1,nO
|
||||
do jb=1,nS
|
||||
eps = w - e(i) + Omega(jb)
|
||||
SigmaC = SigmaC + 2d0*rho(p,i,jb)**2*eps/(eps**2 + eta**2)
|
||||
eps = w - e(i) + Om(jb)
|
||||
GW_SigC = GW_SigC + 2d0*rho(p,i,jb)**2*eps/(eps**2 + eta**2)
|
||||
enddo
|
||||
enddo
|
||||
! Virtual part of the correlation self-energy
|
||||
do a=nO+1,nBas-nR
|
||||
do jb=1,nS
|
||||
eps = w - e(a) - Omega(jb)
|
||||
SigmaC = SigmaC + 2d0*rho(p,a,jb)**2*eps/(eps**2 + eta**2)
|
||||
eps = w - e(a) - Om(jb)
|
||||
GW_SigC = GW_SigC + 2d0*rho(p,a,jb)**2*eps/(eps**2 + eta**2)
|
||||
enddo
|
||||
enddo
|
||||
end if
|
||||
|
||||
end function SigmaC
|
||||
end function
|
@ -1,4 +1,4 @@
|
||||
double precision function dSigmaC(p,w,eta,nBas,nC,nO,nV,nR,nS,e,Omega,rho,regularize)
|
||||
double precision function GW_dSigC(p,w,eta,nBas,nC,nO,nV,nR,nS,e,Om,rho,regularize)
|
||||
|
||||
! Compute the derivative of the correlation part of the self-energy
|
||||
|
||||
@ -17,7 +17,7 @@ double precision function dSigmaC(p,w,eta,nBas,nC,nO,nV,nR,nS,e,Omega,rho,regula
|
||||
integer,intent(in) :: nR
|
||||
integer,intent(in) :: nS
|
||||
double precision,intent(in) :: e(nBas)
|
||||
double precision,intent(in) :: Omega(nS)
|
||||
double precision,intent(in) :: Om(nS)
|
||||
double precision,intent(in) :: rho(nBas,nBas,nS)
|
||||
logical,intent(in) :: regularize
|
||||
|
||||
@ -29,23 +29,23 @@ double precision function dSigmaC(p,w,eta,nBas,nC,nO,nV,nR,nS,e,Omega,rho,regula
|
||||
|
||||
! Initialize
|
||||
|
||||
dSigmaC = 0d0
|
||||
GW_dSigC = 0d0
|
||||
|
||||
if (regularize) then
|
||||
! Occupied part of the correlation self-energy
|
||||
do i=nC+1,nO
|
||||
do jb=1,nS
|
||||
eps = w - e(i) + Omega(jb)
|
||||
Dpijb = e(p) - e(i) + Omega(jb)
|
||||
dSigmaC = dSigmaC - 2d0*rho(p,i,jb)**2*(1d0-exp(-2*eta*Dpijb*Dpijb))/(eps**2)
|
||||
eps = w - e(i) + Om(jb)
|
||||
Dpijb = e(p) - e(i) + Om(jb)
|
||||
GW_dSigC = GW_dSigC - 2d0*rho(p,i,jb)**2*(1d0-exp(-2*eta*Dpijb*Dpijb))/(eps**2)
|
||||
enddo
|
||||
enddo
|
||||
! Virtual part of the correlation self-energy
|
||||
do a=nO+1,nBas-nR
|
||||
do jb=1,nS
|
||||
eps = w - e(a) - Omega(jb)
|
||||
Dpajb = e(p) - e(a) - Omega(jb)
|
||||
dSigmaC = dSigmaC - 2d0*rho(p,a,jb)**2*(1d0-exp(-2*eta*Dpajb*Dpajb))/(eps**2)
|
||||
eps = w - e(a) - Om(jb)
|
||||
Dpajb = e(p) - e(a) - Om(jb)
|
||||
GW_dSigC = GW_dSigC - 2d0*rho(p,a,jb)**2*(1d0-exp(-2*eta*Dpajb*Dpajb))/(eps**2)
|
||||
enddo
|
||||
enddo
|
||||
|
||||
@ -56,8 +56,8 @@ double precision function dSigmaC(p,w,eta,nBas,nC,nO,nV,nR,nS,e,Omega,rho,regula
|
||||
do j=nC+1,nO
|
||||
do b=nO+1,nBas-nR
|
||||
jb = jb + 1
|
||||
eps = w - e(i) + Omega(jb)
|
||||
dSigmaC = dSigmaC - 2d0*rho(p,i,jb)**2*(eps**2 - eta**2)/(eps**2 + eta**2)**2
|
||||
eps = w - e(i) + Om(jb)
|
||||
GW_dSigC = GW_dSigC - 2d0*rho(p,i,jb)**2*(eps**2 - eta**2)/(eps**2 + eta**2)**2
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
@ -68,11 +68,11 @@ double precision function dSigmaC(p,w,eta,nBas,nC,nO,nV,nR,nS,e,Omega,rho,regula
|
||||
do j=nC+1,nO
|
||||
do b=nO+1,nBas-nR
|
||||
jb = jb + 1
|
||||
eps = w - e(a) - Omega(jb)
|
||||
dSigmaC = dSigmaC - 2d0*rho(p,a,jb)**2*(eps**2 - eta**2)/(eps**2 + eta**2)**2
|
||||
eps = w - e(a) - Om(jb)
|
||||
GW_dSigC = GW_dSigC - 2d0*rho(p,a,jb)**2*(eps**2 - eta**2)/(eps**2 + eta**2)**2
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
end if
|
||||
|
||||
end function dSigmaC
|
||||
end function
|
@ -161,7 +161,7 @@ subroutine evGW(maxSCF,thresh,max_diis,doACFDT,exchange_kernel,doXBS,dophBSE,dop
|
||||
write(*,*) ' *** Quasiparticle energies obtained by root search (experimental) *** '
|
||||
write(*,*)
|
||||
|
||||
call QP_graph(nBas,nC,nO,nV,nR,nS,eta,eHF,Om,rho,eGW,eGW,regularize)
|
||||
call GW_QP_graph(nBas,nC,nO,nV,nR,nS,eta,eHF,Om,rho,eGW,eGW,regularize)
|
||||
|
||||
end if
|
||||
|
||||
|
Loading…
Reference in New Issue
Block a user