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qp2/plugins/local/basis_correction/print_routine.irp.f
Anthony Scemama d4d4393956
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cas_ful -> cas_full
2023-11-11 16:13:23 +01:00

83 lines
3.9 KiB
Fortran

subroutine print_basis_correction
implicit none
integer :: istate
provide mu_average_prov
if(mu_of_r_potential.EQ."hf")then
provide ecmd_lda_mu_of_r ecmd_pbe_ueg_mu_of_r
else if(mu_of_r_potential.EQ."cas_full".or.mu_of_r_potential.EQ."cas_truncated")then
provide ecmd_lda_mu_of_r ecmd_pbe_ueg_mu_of_r
provide ecmd_pbe_on_top_mu_of_r ecmd_pbe_on_top_su_mu_of_r
endif
print*, ''
print*, ''
print*, '****************************************'
print*, '****************************************'
print*, 'Basis set correction for WFT using DFT Ecmd functionals'
print*, 'These functionals are accurate for short-range correlation'
print*, ''
print*, 'For more details look at Journal of Chemical Physics 149, 194301 1-15 (2018) '
print*, ' Journal of Physical Chemistry Letters 10, 2931-2937 (2019) '
print*, ' Journal of Chemical Physics 152, 174104 (2020) '
print*, '****************************************'
print*, '****************************************'
print*, 'mu_of_r_potential = ',mu_of_r_potential
if(mu_of_r_potential.EQ."hf")then
print*, ''
print*,'Using a HF-like two-body density to define mu(r)'
print*,'This assumes that HF is a qualitative representation of the wave function '
print*,'********************************************'
print*,'Functionals more suited for weak correlation'
print*,'********************************************'
print*,'+) LDA Ecmd functional : purely based on the UEG (JCP,149,194301,1-15 (2018)) '
do istate = 1, N_states
write(*, '(A29,X,I3,X,A3,X,F16.10)') ' ECMD LDA , state ',istate,' = ',ecmd_lda_mu_of_r(istate)
enddo
print*,'+) PBE-UEG Ecmd functional : PBE at mu=0, UEG ontop pair density at large mu (JPCL, 10, 2931-2937 (2019))'
do istate = 1, N_states
write(*, '(A29,X,I3,X,A3,X,F16.10)') ' ECMD PBE-UEG , state ',istate,' = ',ecmd_pbe_ueg_mu_of_r(istate)
enddo
else if(mu_of_r_potential.EQ."cas_full".or.mu_of_r_potential.EQ."cas_truncated".or.mu_of_r_potential.EQ."pure_act")then
print*, ''
print*,'Using a CAS-like two-body density to define mu(r)'
print*,'This assumes that the CAS is a qualitative representation of the wave function '
print*,'********************************************'
print*,'Functionals more suited for weak correlation'
print*,'********************************************'
print*,'+) LDA Ecmd functional : purely based on the UEG (JCP,149,194301,1-15 (2018)) '
do istate = 1, N_states
write(*, '(A29,X,I3,X,A3,X,F16.10)') ' ECMD LDA , state ',istate,' = ',ecmd_lda_mu_of_r(istate)
enddo
print*,'+) PBE-UEG Ecmd functional : PBE at mu=0, UEG ontop pair density at large mu (JPCL, 10, 2931-2937 (2019))'
do istate = 1, N_states
write(*, '(A29,X,I3,X,A3,X,F16.10)') ' ECMD PBE-UEG , state ',istate,' = ',ecmd_pbe_ueg_mu_of_r(istate)
enddo
print*,''
print*,'********************************************'
print*,'********************************************'
print*,'+) PBE-on-top Ecmd functional : JCP, 152, 174104 (2020) '
print*,'PBE at mu=0, extrapolated ontop pair density at large mu, usual spin-polarization'
do istate = 1, N_states
write(*, '(A29,X,I3,X,A3,X,F16.10)') ' ECMD PBE-OT , state ',istate,' = ',ecmd_pbe_on_top_mu_of_r(istate)
enddo
print*,''
print*,'********************************************'
print*,'+) PBE-on-top no spin polarization Ecmd functional : JCP, 152, 174104 (2020)'
print*,'PBE at mu=0, extrapolated ontop pair density at large mu, and ZERO SPIN POLARIZATION'
do istate = 1, N_states
write(*, '(A29,X,I3,X,A3,X,F16.10)') ' ECMD SU-PBE-OT , state ',istate,' = ',ecmd_pbe_on_top_su_mu_of_r(istate)
enddo
print*,''
endif
print*,''
print*,'**************'
do istate = 1, N_states
write(*, '(A29,X,I3,X,A3,X,F16.10)') ' Average mu(r) , state ',istate,' = ',mu_average_prov(istate)
enddo
end