LCPQ/quantum_package
10
0
Fork 0
mirror of https://github.com/LCPQ/quantum_package synced 2025-01-10 21:18:29 +01:00
Code Issues Releases Wiki Activity

CIS_DT cleaned, add Full_ci/parameters.irp.f

Browse Source
This commit is contained in:
Manu 2014-07-12 12:20:53 +02:00
parent 762fbd41cc
commit 8bb8e1f7c2
9 changed files with 570 additions and 334 deletions
Show Stats Download Patch File Download Diff File Expand all files Collapse all files

68
src/CIS_dressed/CIS_DT_lapack.irp.f Normal file
View File

@ -0,0 +1,68 @@
program CIS_DT
implicit none
integer :: i
print*,'MP2_dresssing=',mp2_dressing
print*,'standard_doubles=',standard_doubles
print*,'n_state_CIS=',n_state_CIS
print*,'n_core_cis=',n_core_cis
print*,'n_act_cis=',n_act_cis
print*,''
print*,'nuc repulsion E=',nuclear_repulsion
if (mp2_dressing==.true.) then
print*,'correlation E=',MP2_corr_energy
else
print*,'correlation E=',EN2_corr_energy
endif
do i = 1,n_state_CIS
print*,''
print*,'i = ',i
print*,'CIS = ',eigenvalues_CIS(i)
print*,'CIS(DdT)= ',eigenvalues_CIS_dress_D_dt(i)
print*,'s2(DdT) = ',s_2_CIS_dress_D_dt(i)
print*,'<x> = ',CIS_states_properties(1,i)
print*,'<y> = ',CIS_states_properties(2,i)
print*,'<z> = ',CIS_states_properties(3,i)
print*,'<xx> = ',CIS_states_properties(4,i)
print*,'<yy> = ',CIS_states_properties(5,i)
print*,'<zz> = ',CIS_states_properties(6,i)
print*,''
enddo
double precision :: delta_E_CIS,delta_E_CIS_DT,convert
convert = 1.d0
print*,'Excitation energies : CIS CIS_DT (Hartree)'
do i = 2, n_state_CIS
delta_E_CIS = eigenvalues_CIS(i) - eigenvalues_CIS(1)
delta_E_CIS_DT = eigenvalues_CIS_dress_D_dt(i) - eigenvalues_CIS_dress_D_dt(1)
write(*,'(I3,xxxxxxxxxxxxxxxx,5(F16.5,x))')i,delta_E_CIS*convert,delta_E_CIS_DT*convert
enddo
convert = 27.2114d0
print*,'Excitation energies : CIS CIS_DT (eV)'
do i = 2, n_state_CIS
delta_E_CIS = eigenvalues_CIS(i) - eigenvalues_CIS(1)
delta_E_CIS_DT = eigenvalues_CIS_dress_D_dt(i) - eigenvalues_CIS_dress_D_dt(1)
write(*,'(I3,xxxxxxxxxxxxxxxx,5(F16.6,x))')i,delta_E_CIS*convert,delta_E_CIS_DT*convert
enddo
convert = 219475d0
print*,'Excitation energies : CIS CIS_DT (cm-1)'
do i = 2, n_state_CIS
delta_E_CIS = eigenvalues_CIS(i) - eigenvalues_CIS(1)
delta_E_CIS_DT = eigenvalues_CIS_dress_D_dt(i) - eigenvalues_CIS_dress_D_dt(1)
write(*,'(I3,xxxxxxxxxxxxxxxx,5(F16.1,x))')i,delta_E_CIS*convert,delta_E_CIS_DT*convert
enddo
convert = 627.51d0
print*,'Excitation energies : CIS CIS_DT (Kcal/mol)'
do i = 2, n_state_CIS
delta_E_CIS = eigenvalues_CIS(i) - eigenvalues_CIS(1)
delta_E_CIS_DT = eigenvalues_CIS_dress_D_dt(i) - eigenvalues_CIS_dress_D_dt(1)
write(*,'(I3,xxxxxxxxxxxxxxxx,5(F16.5,x))')i,delta_E_CIS*convert,delta_E_CIS_DT*convert
enddo
!if(save_all_dm_cis)then
! call save_all_density_matrix
!endif
end

7
src/CIS_dressed/CIS_providers.irp.f
View File

@ -207,13 +207,13 @@
implicit none
double precision,allocatable :: delta_H_matrix_doub(:,:)
double precision,allocatable :: eigvalues(:),eigvectors(:,:)
double precision :: overlap,max_overlap,s2
double precision :: overlap,max_overlap,s2,e_corr
integer :: i_overlap,i,j,k
allocate (delta_H_matrix_doub(size_psi_CIS,size_psi_CIS))
allocate(eigvalues(size_psi_CIS),eigvectors(size_psi_CIS,size_psi_CIS))
do i = 1,n_state_CIS
! call dress_by_doubles(eigenvalues_CIS(i),coefs_CIS(1,i),delta_H_matrix_doub,size_psi_CIS) !dressing of the Doubles
delta_H_matrix_doub = 0.d0
call dress_by_doubles(eigenvalues_CIS(i),coefs_CIS(1,i),delta_H_matrix_doub,size_psi_CIS) !dressing of the Doubles
! delta_H_matrix_doub = 0.d0
do j = 1,size_psi_CIS
do k = 1,size_psi_CIS
@ -246,7 +246,6 @@
enddo
print*,i,i_overlap
print*,'overlap = ',max_overlap
i_overlap = i
overlap_Ddt=max_overlap
do k = 1,size_psi_CIS
eigenvectors_CIS_dress_D_dt(k,i) = eigvectors(k,i_overlap)

465
src/CIS_dressed/EN2.irp.f
View File

@ -1,29 +1,33 @@
BEGIN_PROVIDER [double precision, EN2_corr_energy]
&BEGIN_PROVIDER [double precision, p_imp_EN,(elec_alpha_num+1:n_act_cis)]
&BEGIN_PROVIDER [double precision, h_imp_EN,(n_core_cis+1:elec_alpha_num)]
&BEGIN_PROVIDER [double precision, hp_imp_EN,(n_core_cis+1:elec_alpha_num,elec_alpha_num+1:n_act_cis)]
BEGIN_DOC
!Calculation of the EN2 correlation energy (EN2_corr_energy)
!and calculation of the contribution of the disconnected Triples on the
!Singles, via the impossible (p_imp_EN, h_imp_EN, hp_imp_EN)
END_DOC
implicit none
integer :: i,j,k,l !variables for going over the occupied (i,j) and virutal (k,l)
double precision :: direct,exchg,hij !calculating direct, exchange and total contribution
double precision :: get_mo_bielec_integral
double precision :: e_i,e_k,e_j,e_l !epsilons of i,j,k,l
double precision :: delta_e_ik,delta_e_ikj
double precision :: delta_e !delta epsilons
double precision :: delta_e_tmp,H_jj_total
integer :: ispin1,ispin2,i_ok
print*,'EN2_corr_energy'
EN2_corr_energy=0.d0
BEGIN_PROVIDER [double precision, EN2_corr_energy]
&BEGIN_PROVIDER [double precision, p_imp_EN,(elec_alpha_num+1:n_act_cis)]
&BEGIN_PROVIDER [double precision, h_imp_EN,(n_core_cis+1:elec_alpha_num)]
&BEGIN_PROVIDER [double precision, hp_imp_EN,(n_core_cis+1:elec_alpha_num,elec_alpha_num+1:n_act_cis)]
BEGIN_DOC
!Calculation of the EN2 correlation energy (EN2_corr_energy)
!and calculation of the contribution of the disconnected Triples on the
!Singles, via the impossible (p_imp_EN, h_imp_EN, hp_imp_EN)
END_DOC
implicit none
integer :: i,j,k,l !variables for going over the occupied (i,j) and virutal (k,l)
double precision :: direct,exchg,hij !calculating direct, exchange and total contribution
double precision :: get_mo_bielec_integral
double precision :: e_i,e_k,e_j,e_l !epsilons of i,j,k,l
double precision :: delta_e_ik,delta_e_ikj
double precision :: delta_e !delta epsilons
double precision :: delta_e_tmp,H_jj_total
integer, allocatable :: key_in(:,:)
integer, allocatable :: key_out(:,:)
integer :: ispin1,ispin2,i_ok
allocate(key_in(N_int,2))
allocate(key_out(N_int,2))
print*,'EN2_corr_energy'
EN2_corr_energy=0.d0
do i=n_core_cis+1,elec_alpha_num
h_imp_EN(i)=0.d0
do k =elec_beta_num + 1, n_act_cis
@ -31,222 +35,209 @@
hp_imp_EN(i,k)=0.d0
enddo
enddo
print*,'HF_energy = ',HF_energy
print*,'1'
if(EN_2_2)then
do i=n_core_cis+1,elec_alpha_num
h_imp_EN(i)=0.d0
e_i=diagonal_Fock_matrix_mo(i)
do k=elec_alpha_num+1,n_act_cis
hp_imp_EN(i,k)=0.d0
if(EN_2_2)then
do i=n_core_cis+1,elec_alpha_num
e_i=Fock_matrix_diag_mo(i)
do k=elec_alpha_num+1,n_act_cis
e_k=Fock_matrix_diag_mo(k)
delta_e_ik=e_i-e_k
e_k=diagonal_Fock_matrix_mo(k)
delta_e_ik=e_i-e_k
!same spin contribution for EN2_corr_energy
do j=i+1,elec_alpha_num
e_j=diagonal_Fock_matrix_mo(j)
delta_e_ikj=delta_e_ik+e_j
!same spin contribution for EN2_corr_energy and a part of the contribution to p_imp_EN,h_imp_EN
do l=k+1,n_act_cis
e_l=diagonal_Fock_matrix_mo(l)
delta_e=delta_e_ikj-e_l
delta_e=delta_e-mo_bielec_integral_jj_anti(i,j) - &
mo_bielec_integral_jj_anti(k,l)
delta_e=delta_e+mo_bielec_integral_jj_anti(i,k) + &
mo_bielec_integral_jj_anti(i,l) + &
mo_bielec_integral_jj_anti(j,k) + &
mo_bielec_integral_jj_anti(j,l)
!
direct=get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
exchg=get_mo_bielec_integral(i,j,l,k,mo_integrals_map)
hij=(direct-exchg)*(direct-exchg)
hij=0.5d0*(-delta_e-dsqrt(delta_e*delta_e+4.d0*hij))
EN2_corr_energy=EN2_corr_energy+2*hij
p_imp_EN(k)=p_imp_EN(k)+hij
h_imp_EN(i)=h_imp_EN(i)+hij
p_imp_EN(l)=p_imp_EN(l)+hij
h_imp_EN(j)=h_imp_EN(j)+hij
enddo
enddo
!same spin contribution for hp_imp_EN
do j=n_core_cis+1,elec_alpha_num
if(j==i)cycle
e_j=diagonal_Fock_matrix_mo(j)
delta_e_ikj=delta_e_ik+e_j
do l=elec_alpha_num+1,n_act_cis
if(l==k)cycle
e_l=diagonal_Fock_matrix_mo(l)
delta_e=delta_e_ikj-e_l
delta_e=delta_e-mo_bielec_integral_jj_anti(i,j) - &
mo_bielec_integral_jj_anti(k,l)
delta_e=delta_e+mo_bielec_integral_jj_anti(i,k) + &
mo_bielec_integral_jj_anti(i,l) + &
mo_bielec_integral_jj_anti(j,k) + &
mo_bielec_integral_jj_anti(j,l)
direct=get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
exchg=get_mo_bielec_integral(i,j,l,k,mo_integrals_map)
hij=(direct-exchg)*(direct-exchg)
hij = 0.5d0 * (-delta_e - dsqrt(delta_e * delta_e + 4.d0 * hij))
hp_imp_EN(i,k)=hp_imp_EN(i,k)+hij
enddo
enddo
!different spin contribution
do j=n_core_cis+1,elec_beta_num
e_j=diagonal_Fock_matrix_mo(j)
delta_e_ikj=delta_e_ik+e_j
do l=elec_beta_num+1,n_act_cis
e_l=diagonal_Fock_matrix_mo(l)
delta_e=delta_e_ikj-e_l
delta_e=delta_e-mo_bielec_integral_jj(i,j) - &
mo_bielec_integral_jj(k,l)
delta_e=delta_e+mo_bielec_integral_jj_anti(i,k) + &
mo_bielec_integral_jj_anti(j,l) + &
mo_bielec_integral_jj(i,l) + &
mo_bielec_integral_jj(j,k)
direct=get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
hij=direct*direct
hij=0.5d0*(-delta_e-dsqrt(delta_e*delta_e+4.d0*hij))
EN2_corr_energy=EN2_corr_energy+hij
p_imp_EN(k)=p_imp_EN(k)+hij
h_imp_EN(i)=h_imp_EN(i)+hij
hp_imp_EN(i,k)=hp_imp_EN(i,k)+hij
enddo
enddo
enddo
enddo
print*,'2'
else
do i=n_core_cis+1,elec_alpha_num
h_imp_EN(i)=0.d0
e_i=diagonal_Fock_matrix_mo(i)
do k=elec_alpha_num+1,n_act_cis
hp_imp_EN(i,k)=0.d0
!same spin contribution for EN2_corr_energy
do j=i+1,elec_alpha_num
e_j=Fock_matrix_diag_mo(j)
delta_e_ikj=delta_e_ik+e_j
e_k=diagonal_Fock_matrix_mo(k)
delta_e_ik=e_i-e_k
!same spin contribution for EN2_corr_energy
do j=i+1,elec_alpha_num
e_j=diagonal_Fock_matrix_mo(j)
delta_e_ikj=delta_e_ik+e_j
!same spin contribution for EN2_corr_energy and a part of the contribution to p_imp_EN,h_imp_EN
do l=k+1,n_act_cis
e_l=diagonal_Fock_matrix_mo(l)
delta_e=delta_e_ikj-e_l
delta_e=delta_e-mo_bielec_integral_jj_anti(i,j) - &
mo_bielec_integral_jj_anti(k,l)
delta_e=delta_e+mo_bielec_integral_jj_anti(i,k) + &
mo_bielec_integral_jj_anti(i,l) + &
mo_bielec_integral_jj_anti(j,k) + &
mo_bielec_integral_jj_anti(j,l)
!
direct=get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
exchg=get_mo_bielec_integral(i,j,l,k,mo_integrals_map)
hij=(direct-exchg)*(direct-exchg)
hij = hij*hij/delta_e
EN2_corr_energy=EN2_corr_energy+2*hij
p_imp_EN(k)=p_imp_EN(k)+hij
h_imp_EN(i)=h_imp_EN(i)+hij
p_imp_EN(l)=p_imp_EN(l)+hij
h_imp_EN(j)=h_imp_EN(j)+hij
!same spin contribution for EN2_corr_energy and a part of the contribution to p_imp_EN,h_imp_EN
do l=k+1,n_act_cis
e_l=Fock_matrix_diag_mo(l)
delta_e=delta_e_ikj-e_l
delta_e=delta_e-mo_bielec_integral_jj_anti(i,j) - &
mo_bielec_integral_jj_anti(k,l)
delta_e=delta_e+mo_bielec_integral_jj_anti(i,k) + &
mo_bielec_integral_jj_anti(i,l) + &
mo_bielec_integral_jj_anti(j,k) + &
mo_bielec_integral_jj_anti(j,l)
!
direct=get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
exchg=get_mo_bielec_integral(i,j,l,k,mo_integrals_map)
hij=(direct-exchg)*(direct-exchg)
hij=0.5d0*(-delta_e-dsqrt(delta_e*delta_e+4.d0*hij))
EN2_corr_energy=EN2_corr_energy+2*hij
p_imp_EN(k)=p_imp_EN(k)+hij
h_imp_EN(i)=h_imp_EN(i)+hij
p_imp_EN(l)=p_imp_EN(l)+hij
h_imp_EN(j)=h_imp_EN(j)+hij
enddo
enddo
!same spin contribution for hp_imp_EN
do j=n_core_cis+1,elec_alpha_num
if(j==i)cycle
e_j=Fock_matrix_diag_mo(j)
delta_e_ikj=delta_e_ik+e_j
do l=elec_alpha_num+1,n_act_cis
if(l==k)cycle
e_l=Fock_matrix_diag_mo(l)
delta_e=delta_e_ikj-e_l
delta_e=delta_e-mo_bielec_integral_jj_anti(i,j) - &
mo_bielec_integral_jj_anti(k,l)
delta_e=delta_e+mo_bielec_integral_jj_anti(i,k) + &
mo_bielec_integral_jj_anti(i,l) + &
mo_bielec_integral_jj_anti(j,k) + &
mo_bielec_integral_jj_anti(j,l)
direct=get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
exchg=get_mo_bielec_integral(i,j,l,k,mo_integrals_map)
hij=(direct-exchg)*(direct-exchg)
hij = 0.5d0 * (-delta_e - dsqrt(delta_e * delta_e + 4.d0 * hij))
hp_imp_EN(i,k)=hp_imp_EN(i,k)+hij
enddo
enddo
!different spin contribution
do j=n_core_cis+1,elec_beta_num
e_j=Fock_matrix_diag_mo(j)
delta_e_ikj=delta_e_ik+e_j
do l=elec_beta_num+1,n_act_cis
e_l=Fock_matrix_diag_mo(l)
delta_e=delta_e_ikj-e_l
delta_e=delta_e-mo_bielec_integral_jj(i,j) - &
mo_bielec_integral_jj(k,l)
delta_e=delta_e+mo_bielec_integral_jj_anti(i,k) + &
mo_bielec_integral_jj_anti(j,l) + &
mo_bielec_integral_jj(i,l) + &
mo_bielec_integral_jj(j,k)
direct=get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
hij=direct*direct
hij=0.5d0*(-delta_e-dsqrt(delta_e*delta_e+4.d0*hij))
EN2_corr_energy=EN2_corr_energy+hij
p_imp_EN(k)=p_imp_EN(k)+hij
h_imp_EN(i)=h_imp_EN(i)+hij
hp_imp_EN(i,k)=hp_imp_EN(i,k)+hij
enddo
enddo
enddo
enddo
!same spin contribution for hp_imp_EN
do j=n_core_cis+1,elec_alpha_num
if(j==i)cycle
e_j=diagonal_Fock_matrix_mo(j)
delta_e_ikj=delta_e_ik+e_j
else
do i=n_core_cis+1,elec_alpha_num
e_i=Fock_matrix_diag_mo(i)
do k=elec_alpha_num+1,n_act_cis
e_k=Fock_matrix_diag_mo(k)
delta_e_ik=e_i-e_k
!same spin contribution for EN2_corr_energy
do j=i+1,elec_alpha_num
e_j=Fock_matrix_diag_mo(j)
delta_e_ikj=delta_e_ik+e_j
!same spin contribution for EN2_corr_energy and a part of the contribution to p_imp_EN,h_imp_EN
do l=k+1,n_act_cis
e_l=Fock_matrix_diag_mo(l)
delta_e=delta_e_ikj-e_l
delta_e=delta_e-mo_bielec_integral_jj_anti(i,j) - &
mo_bielec_integral_jj_anti(k,l)
delta_e=delta_e+mo_bielec_integral_jj_anti(i,k) + &
mo_bielec_integral_jj_anti(i,l) + &
mo_bielec_integral_jj_anti(j,k) + &
mo_bielec_integral_jj_anti(j,l)
!
direct=get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
exchg=get_mo_bielec_integral(i,j,l,k,mo_integrals_map)
hij=(direct-exchg)*(direct-exchg)
hij=hij/delta_e
EN2_corr_energy=EN2_corr_energy+2*hij
p_imp_EN(k)=p_imp_EN(k)+hij
h_imp_EN(i)=h_imp_EN(i)+hij
p_imp_EN(l)=p_imp_EN(l)+hij
h_imp_EN(j)=h_imp_EN(j)+hij
enddo
enddo
!same spin contribution for hp_imp_EN
do j=n_core_cis+1,elec_alpha_num
if(j==i)cycle
e_j=Fock_matrix_diag_mo(j)
delta_e_ikj=delta_e_ik+e_j
do l=elec_alpha_num+1,n_act_cis
if(l==k)cycle
e_l=Fock_matrix_diag_mo(l)
delta_e=delta_e_ikj-e_l
delta_e=delta_e-mo_bielec_integral_jj_anti(i,j) - &
mo_bielec_integral_jj_anti(k,l)
delta_e=delta_e+mo_bielec_integral_jj_anti(i,k) + &
mo_bielec_integral_jj_anti(i,l) + &
mo_bielec_integral_jj_anti(j,k) + &
mo_bielec_integral_jj_anti(j,l)
direct=get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
exchg=get_mo_bielec_integral(i,j,l,k,mo_integrals_map)
hij=(direct-exchg)*(direct-exchg)
hij=hij/delta_e
hp_imp_EN(i,k)=hp_imp_EN(i,k)+hij
enddo
enddo
!different spin contribution
do j=n_core_cis+1,elec_beta_num
e_j=Fock_matrix_diag_mo(j)
delta_e_ikj=delta_e_ik+e_j
do l=elec_beta_num+1,n_act_cis
e_l=Fock_matrix_diag_mo(l)
delta_e=delta_e_ikj-e_l
delta_e=delta_e-mo_bielec_integral_jj(i,j) - &
mo_bielec_integral_jj(k,l)
delta_e=delta_e+mo_bielec_integral_jj_anti(i,k) + &
mo_bielec_integral_jj_anti(j,l) + &
mo_bielec_integral_jj(i,l) + &
mo_bielec_integral_jj(j,k)
direct=get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
hij=direct*direct
hij=hij/delta_e
EN2_corr_energy=EN2_corr_energy+hij
p_imp_EN(k)=p_imp_EN(k)+hij
h_imp_EN(i)=h_imp_EN(i)+hij
hp_imp_EN(i,k)=hp_imp_EN(i,k)+hij
enddo
enddo
enddo
enddo
endif
do l=elec_alpha_num+1,n_act_cis
if(l==k)cycle
e_l=diagonal_Fock_matrix_mo(l)
delta_e=delta_e_ikj-e_l
delta_e=delta_e-mo_bielec_integral_jj_anti(i,j) - &
mo_bielec_integral_jj_anti(k,l)
delta_e=delta_e+mo_bielec_integral_jj_anti(i,k) + &
mo_bielec_integral_jj_anti(i,l) + &
mo_bielec_integral_jj_anti(j,k) + &
mo_bielec_integral_jj_anti(j,l)
direct=get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
exchg=get_mo_bielec_integral(i,j,l,k,mo_integrals_map)
hij=(direct-exchg)*(direct-exchg)
hij = hij*hij/delta_e
hp_imp_EN(i,k)=hp_imp_EN(i,k)+hij
enddo
enddo
!different spin contribution
do j=n_core_cis+1,elec_beta_num
e_j=diagonal_Fock_matrix_mo(j)
delta_e_ikj=delta_e_ik+e_j
do l=elec_beta_num+1,n_act_cis
e_l=diagonal_Fock_matrix_mo(l)
delta_e=delta_e_ikj-e_l
delta_e=delta_e-mo_bielec_integral_jj(i,j) - &
mo_bielec_integral_jj(k,l)
delta_e=delta_e+mo_bielec_integral_jj_anti(i,k) + &
mo_bielec_integral_jj_anti(j,l) + &
mo_bielec_integral_jj(i,l) + &
mo_bielec_integral_jj(j,k)
direct=get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
hij=direct*direct
hij = hij*hij/delta_e
EN2_corr_energy=EN2_corr_energy+hij
p_imp_EN(k)=p_imp_EN(k)+hij
h_imp_EN(i)=h_imp_EN(i)+hij
hp_imp_EN(i,k)=hp_imp_EN(i,k)+hij
enddo
enddo
enddo
enddo
endif
print*,'EN correlation energy=',EN2_corr_energy
print*,'EN correlation energy=',EN2_corr_energy
END_PROVIDER
print*,'EN correlation energy=',EN2_corr_energy
print*,'EN correlation energy=',EN2_corr_energy
END_PROVIDER

127
src/CIS_dressed/MP2.irp.f
View File

@ -29,22 +29,22 @@
do i=n_core_cis+1,elec_alpha_num
h_imp(i)=0.d0
e_i=diagonal_Fock_matrix_mo(i)
e_i=Fock_matrix_diag_mo(i)
do k=elec_alpha_num+1,n_act_cis
hp_imp(i,k)=0.d0
e_k=diagonal_Fock_matrix_mo(k)
e_k=Fock_matrix_diag_mo(k)
delta_e_ik=e_i-e_k
!same spin contribution for MP2_corr_energy
do j=i+1,elec_alpha_num
e_j=diagonal_Fock_matrix_mo(j)
e_j=Fock_matrix_diag_mo(j)
delta_e_ikj=delta_e_ik+e_j
!same spin contribution for MP2_corr_energy and a part of the contribution to p_imp and h_imp
do l=k+1,n_act_cis
e_l=diagonal_Fock_matrix_mo(l)
e_l=Fock_matrix_diag_mo(l)
delta_e=delta_e_ikj-e_l
direct=get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
@ -60,7 +60,7 @@
!remaining same spin contribution for p_imp
do l=elec_alpha_num+1,k-1
e_l=diagonal_Fock_matrix_mo(l)
e_l=Fock_matrix_diag_mo(l)
delta_e=delta_e_ikj-e_l
direct=get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
@ -75,11 +75,11 @@
!remaining same spin contribution for h_imp
do j=n_core_cis+1,i-1
e_j=diagonal_Fock_matrix_mo(j)
e_j=Fock_matrix_diag_mo(j)
delta_e_ikj=delta_e_ik+e_j
do l=k+1,n_act_cis
e_l=diagonal_Fock_matrix_mo(l)
e_l=Fock_matrix_diag_mo(l)
delta_e=delta_e_ikj-e_l
direct=get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
@ -94,11 +94,11 @@
!same spin contribution for hp_imp
do j=n_core_cis+1,elec_alpha_num
e_j=diagonal_Fock_matrix_mo(j)
e_j=Fock_matrix_diag_mo(j)
delta_e_ikj=delta_e_ik+e_j
do l=elec_alpha_num+1,n_act_cis
e_l=diagonal_Fock_matrix_mo(l)
e_l=Fock_matrix_diag_mo(l)
delta_e=delta_e_ikj-e_l
direct=get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
@ -113,11 +113,11 @@
!different spin contribution
do j=n_core_cis+1,elec_beta_num
e_j=diagonal_Fock_matrix_mo(j)
e_j=Fock_matrix_diag_mo(j)
delta_e_ikj=delta_e_ik+e_j
do l=elec_beta_num+1,n_act_cis
e_l=diagonal_Fock_matrix_mo(l)
e_l=Fock_matrix_diag_mo(l)
delta_e=delta_e_ikj-e_l
direct=get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
@ -385,25 +385,20 @@
enddo
else !EN Dressing
print*,'coucou !'
dress_T_discon_array_CIS(1)=EN2_corr_energy
print*,'coucou !'
! do i=n_core_cis+1,elec_alpha_num
! print*,'i',i,n_core_cis
! do k=elec_alpha_num+1,n_act_cis
! print*,'k',k,n_act_cis
! key=psi_CIS_adress(i,k)
!
! dress_T_discon(i,k)=EN2_corr_energy-p_imp_EN(k)-h_imp_EN(i)+hp_imp_EN(i,k)
do i=n_core_cis+1,elec_alpha_num
do k=elec_alpha_num+1,n_act_cis
key=psi_CIS_adress(i,k)
dress_T_discon(i,k)=EN2_corr_energy-p_imp_EN(k)-h_imp_EN(i)+hp_imp_EN(i,k)
! dress_T_discon_array_CIS(key) = dress_T_discon(i,k)
! dress_T_discon_array_CIS(key+1) = dress_T_discon(i,k)
dress_T_discon_array_CIS(key) = dress_T_discon(i,k)
dress_T_discon_array_CIS(key+1) = dress_T_discon(i,k)
! enddo
! enddo
enddo
enddo
end if
print*,'end'
END_PROVIDER
@ -809,24 +804,24 @@
delta_H_trip=0.d0
!do i=5,6
do i=n_core_cis+1,elec_alpha_num
e_i=diagonal_Fock_matrix_mo(i)
e_i=Fock_matrix_diag_mo(i)
!r=7
do r=elec_alpha_num+1,n_act_cis
e_r=diagonal_Fock_matrix_mo(r)
e_r=Fock_matrix_diag_mo(r)
delta_e_ir=e_i-e_r
key_ir=psi_CIS_adress(i,r)
do j=i+1,elec_alpha_num
e_j=diagonal_Fock_matrix_mo(j)
e_j=Fock_matrix_diag_mo(j)
delta_e_irj=delta_e_ir+e_j
do s=r+1,n_act_cis
e_s=diagonal_Fock_matrix_mo(s)
e_s=Fock_matrix_diag_mo(s)
delta_e_irjs=delta_e_irj-e_s
!alpha-alpha-alpha
do k=j+1,elec_alpha_num
e_k=diagonal_Fock_matrix_mo(k)
e_k=Fock_matrix_diag_mo(k)
delta_e_irjsk=delta_e_irjs+e_k
do t=s+1,n_act_cis
e_t=diagonal_Fock_matrix_mo(t)
e_t=Fock_matrix_diag_mo(t)
delta_e=delta_e_irjsk-e_t
energy=1.d0/(ref_energy-delta_e)
occ=i
@ -898,10 +893,10 @@
enddo
!alpha-alpha-beta
do k=n_core_cis+1,elec_alpha_num
e_k=diagonal_Fock_matrix_mo(k)
e_k=Fock_matrix_diag_mo(k)
delta_e_irjsk=delta_e_irjs+e_k
do t=elec_alpha_num+1,n_act_cis
e_t=diagonal_Fock_matrix_mo(t)
e_t=Fock_matrix_diag_mo(t)
delta_e=delta_e_irjsk-e_t
energy=1.d0/(ref_energy-delta_e)
occ=i
@ -992,23 +987,23 @@
!!generating the Singles included in the Triples
!! do m=1,n_state_CIS
!do i=n_core_cis+1,elec_alpha_num
! e_i=diagonal_Fock_matrix_mo(i)
! e_i=Fock_matrix_diag_mo(i)
!!do r=elec_alpha_num+1,n_state_CIS
! do r=elec_alpha_num+1,n_act_cis
! e_r=diagonal_Fock_matrix_mo(r)
! e_r=Fock_matrix_diag_mo(r)
! delta_e_ir=e_i-e_r
!key_ir=psi_CIS_adress(i,r)
! !alpha-alpha-x (=beta-beta-x)
! do j=i+1,elec_alpha_num
! e_j=diagonal_Fock_matrix_mo(j)
! e_j=Fock_matrix_diag_mo(j)
! delta_e_irj=delta_e_ir+e_j
!key_jr=psi_CIS_adress(j,r)
! do s=r+1,n_act_cis
! e_s=diagonal_Fock_matrix_mo(s)
! e_s=Fock_matrix_diag_mo(s)
! delta_e_irjs=delta_e_irj-e_s
! key_is=psi_CIS_adress(i,s)
@ -1017,13 +1012,13 @@
! !alpha-alpha-alpha (=beta-beta-beta)
! do k=j+1,elec_alpha_num
! e_k=diagonal_Fock_matrix_mo(k)
! e_k=Fock_matrix_diag_mo(k)
! delta_e_irjsk=delta_e_irjs+e_k
! key_kr=psi_CIS_adress(k,r)
! key_ks=psi_CIS_adress(k,s)
! do t=s+1,n_act_cis
! e_t=diagonal_Fock_matrix_mo(t)
! e_t=Fock_matrix_diag_mo(t)
! delta_e=delta_e_irjsk-e_t
! key_it=psi_CIS_adress(i,t)
@ -1157,7 +1152,7 @@
! !alpha-alpha-beta (=beta-beta-alpha)
! do k=n_core_cis+1,elec_beta_num
! e_k=diagonal_Fock_matrix_mo(k)
! e_k=Fock_matrix_diag_mo(k)
! delta_e_irjsk=delta_e_irjs+e_k
! key_kr=psi_CIS_adress(k,r)
@ -1166,7 +1161,7 @@
! do t=elec_beta_num+1,n_act_cis
! e_t=diagonal_Fock_matrix_mo(t)
! e_t=Fock_matrix_diag_mo(t)
! delta_e=delta_e_irjsk-e_t
! key_it=psi_CIS_adress(i,t)
@ -1298,53 +1293,3 @@
!enddo
END
subroutine diexcitation(i,j,k,l,ispin1,ispin2,key_in,key_out,i_ok,Nint)
implicit none
use bitmasks
! realize the double excitation i-->k (ispin1) + j-->l (ispin2) on key_in
! returns key_out and i_ok (i_ok = 0 means not possible, i_ok = 1 means the excitation was possible)
integer, intent(in) :: ispin1,ispin2,i,j,k,l,Nint
integer(bit_kind), intent(in) :: key_in(Nint,2)
integer, intent(out):: i_ok
integer(bit_kind), intent(out):: key_out(Nint,2)
integer :: k_hole,j_hole,k_particl,j_particl,i_nint,Nelec_alpha,Nelec_beta
integer :: i_test_hole,i_test_particl
key_out = key_in
k_hole = ishft(i-1,-bit_kind_shift)+1
j_hole = i-ishft(k_hole-1,bit_kind_shift)-1
i_test_hole = ibset(0,j_hole)
if(iand(key_in(k_hole,ispin1),i_test_hole).ne.i_test_hole)then
i_ok = 0
return
endif
key_out(k_hole,ispin1) = ibclr(key_out(k_hole,ispin1),j_hole)
k_particl = ishft(k-1,-bit_kind_shift)+1
j_particl = k-ishft(k_particl-1,bit_kind_shift)-1
i_test_particl= ibset(0,j_particl)
if(iand(key_in(k_particl,ispin1),i_test_particl).ne.0)then
i_ok = 0
return
endif
key_out(k_particl,ispin1) = ibset(key_out(k_particl,ispin1),j_particl)
k_hole = ishft(j-1,-bit_kind_shift)+1
j_hole = j-ishft(k_hole-1,bit_kind_shift)-1
i_test_hole = ibset(0,j_hole)
if(iand(key_in(k_hole,ispin2),i_test_hole).ne.i_test_hole)then
i_ok = 0
return
endif
key_out(k_hole,ispin2) = ibclr(key_out(k_hole,ispin2),j_hole)
k_particl = ishft(l-1,-bit_kind_shift)+1
j_particl = l-ishft(k_particl-1,bit_kind_shift)-1
i_test_particl = ibset(0,j_particl)
if(iand(key_in(k_particl,ispin2),i_test_particl).ne.0)then
i_ok = 0
return
endif
key_out(k_particl,ispin2) = ibset(key_out(k_particl,ispin2),j_particl)
i_ok = 1
end

2
src/CIS_dressed/natural_particl_orbitals.irp.f
View File

@ -56,7 +56,7 @@
enddo
do k = 1, mo_tot_num
do l = 1, mo_tot_num
c_k = eigvectors(k,j) * eigvectors(l,j)
c_k = eigvectors(k,i) * eigvectors(l,i)
particle_natural_orb_CIS_properties(1,i) += c_k * mo_dipole_x(k,l)
particle_natural_orb_CIS_properties(2,i) += c_k * mo_dipole_y(k,l)
particle_natural_orb_CIS_properties(3,i) += c_k * mo_dipole_z(k,l)

3
src/CIS_dressed/options.irp.f
View File

@ -10,7 +10,8 @@ BEGIN_PROVIDER [ integer , n_state_cis ]
if (has) then
call ezfio_get_cis_dressed_n_state_cis(n_state_cis)
else
n_state_cis = 5
n_state_cis = 10
call ezfio_set_cis_dressed_n_state_cis(n_state_cis)
endif
END_PROVIDER

178
src/CIS_dressed/repeat_all_doubles.irp.f Normal file
View File

@ -0,0 +1,178 @@
subroutine repeat_all_doubles(key_in, e_corr)
implicit none
integer(bit_kind), intent(in) :: key_in(N_int,2)
double precision, intent(out) :: e_corr
integer :: i,j,k,l
integer :: s1,s2
integer :: i_ok
double precision :: hij,get_mo_bielec_integral,diag_H_mat_elem,delta_e
integer(bit_kind) :: key_out(N_int,2)
! same spin (alpha)
if(mp2_dressing)then
s1 = 1
e_corr = 0.d0
do i = n_core_cis + 1, elec_alpha_num
do j = i + 1, elec_alpha_num
do k = elec_alpha_num + 1, n_act_cis
do l = k+1, n_act_cis
! a^+ k(s1) a^+ l(s1) a_j(s1) a_i(s1) |key_in>
call diexcitation(i,j,k,l,s1,s1,key_in,key_out,i_ok,N_int)
if(i_ok.ne.0)then
hij = get_mo_bielec_integral(i,j,k,l,mo_integrals_map) &
-get_mo_bielec_integral(i,j,l,k,mo_integrals_map)
e_corr += hij*hij/(Fock_matrix_diag_mo(i)+Fock_matrix_diag_mo(j) &
-Fock_matrix_diag_mo(l)-Fock_matrix_diag_mo(k))
endif
enddo
enddo
enddo
enddo
s1 = 2
do i = n_core_cis + 1, elec_alpha_num
do j = i + 1, elec_alpha_num
do k = elec_alpha_num + 1, n_act_cis
do l = k+1, n_act_cis
! a^+ k(s1) a^+ l(s1) a_j(s1) a_i(s1) |key_in>
call diexcitation(i,j,k,l,s1,s1,key_in,key_out,i_ok,N_int)
if(i_ok.ne.0)then
hij = get_mo_bielec_integral(i,j,k,l,mo_integrals_map) &
-get_mo_bielec_integral(i,j,l,k,mo_integrals_map)
e_corr += hij*hij/(Fock_matrix_diag_mo(i)+Fock_matrix_diag_mo(j) &
-Fock_matrix_diag_mo(l)-Fock_matrix_diag_mo(k))
endif
enddo
enddo
enddo
enddo
s1 = 1
s2 = 2
do i = n_core_cis + 1, elec_alpha_num
do j = n_core_cis + 1, elec_alpha_num
do k = elec_alpha_num + 1, n_act_cis
do l = elec_alpha_num + 1, n_act_cis
! a^+ k(s1) a^+ l(s1) a_j(s1) a_i(s1) |key_in>
call diexcitation(i,j,k,l,s1,s2,key_in,key_out,i_ok,N_int)
if(i_ok.ne.0)then
hij = get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
e_corr += hij*hij/(Fock_matrix_diag_mo(i)+Fock_matrix_diag_mo(j) &
-Fock_matrix_diag_mo(l)-Fock_matrix_diag_mo(k))
endif
enddo
enddo
enddo
enddo
else
! same spin (alpha)
s1 = 1
e_corr = 0.d0
do i = n_core_cis + 1, elec_alpha_num
do j = i + 1, elec_alpha_num
do k = elec_alpha_num + 1, n_act_cis
do l = k+1, n_act_cis
! a^+ k(s1) a^+ l(s1) a_j(s1) a_i(s1) |key_in>
call diexcitation(i,j,k,l,s1,s1,key_in,key_out,i_ok,N_int)
if(i_ok.ne.0)then
hij = get_mo_bielec_integral(i,j,k,l,mo_integrals_map) &
-get_mo_bielec_integral(i,j,l,k,mo_integrals_map)
call diexcitation(i,j,k,l,s1,s1,ref_bitmask,key_out,i_ok,N_int)
delta_e = HF_energy - diag_H_mat_elem(key_out,N_int)
e_corr += hij*hij/delta_e
endif
enddo
enddo
enddo
enddo
s1 = 2
do i = n_core_cis + 1, elec_alpha_num
do j = i + 1, elec_alpha_num
do k = elec_alpha_num + 1, n_act_cis
do l = k+1, n_act_cis
! a^+ k(s1) a^+ l(s1) a_j(s1) a_i(s1) |key_in>
call diexcitation(i,j,k,l,s1,s1,key_in,key_out,i_ok,N_int)
if(i_ok.ne.0)then
hij = get_mo_bielec_integral(i,j,k,l,mo_integrals_map) &
-get_mo_bielec_integral(i,j,l,k,mo_integrals_map)
call diexcitation(i,j,k,l,s1,s1,ref_bitmask,key_out,i_ok,N_int)
delta_e = HF_energy - diag_H_mat_elem(key_out,N_int)
e_corr += hij*hij/delta_e
endif
enddo
enddo
enddo
enddo
s1 = 1
s2 = 2
do i = n_core_cis + 1, elec_alpha_num
do j = n_core_cis + 1, elec_alpha_num
do k = elec_alpha_num + 1, n_act_cis
do l = elec_alpha_num + 1, n_act_cis
! a^+ k(s1) a^+ l(s1) a_j(s1) a_i(s1) |key_in>
call diexcitation(i,j,k,l,s1,s2,key_in,key_out,i_ok,N_int)
if(i_ok.ne.0)then
hij = get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
call diexcitation(i,j,k,l,s1,s2,ref_bitmask,key_out,i_ok,N_int)
delta_e = HF_energy - diag_H_mat_elem(key_out,N_int)
e_corr += hij*hij/delta_e
endif
enddo
enddo
enddo
enddo
endif
end
subroutine diexcitation(i,j,k,l,ispin1,ispin2,key_in,key_out,i_ok,Nint)
implicit none
use bitmasks
! realize the double excitation i-->k (ispin1) + j-->l (ispin2) on key_in
! returns key_out and i_ok (i_ok = 0 means not possible, i_ok = 1 means the excitation was possible)
integer, intent(in) :: ispin1,ispin2,i,j,k,l,Nint
integer(bit_kind), intent(in) :: key_in(Nint,2)
integer, intent(out):: i_ok
integer(bit_kind), intent(out):: key_out(Nint,2)
integer :: k_hole,j_hole,k_particl,j_particl,i_nint,Nelec_alpha,Nelec_beta
integer(bit_kind) :: i_test_hole,i_test_particl
character*(512) :: output(2)
key_out = key_in
k_hole = ishft(i-1,-bit_kind_shift)+1
j_hole = i-ishft(k_hole-1,bit_kind_shift)-1
i_test_hole = ibset(0_bit_kind,j_hole)
if(iand(key_in(k_hole,ispin1),i_test_hole).ne.i_test_hole)then
i_ok = 0
return
endif
key_out(k_hole,ispin1) = ibclr(key_out(k_hole,ispin1),j_hole)
k_particl = ishft(k-1,-bit_kind_shift)+1
j_particl = k-ishft(k_particl-1,bit_kind_shift)-1
i_test_particl= ibset(0_bit_kind,j_particl)
if(iand(key_in(k_particl,ispin1),i_test_particl).ne.0_bit_kind)then
i_ok = 0
return
endif
key_out(k_particl,ispin1) = ibset(key_out(k_particl,ispin1),j_particl)
k_hole = ishft(j-1,-bit_kind_shift)+1
j_hole = j-ishft(k_hole-1,bit_kind_shift)-1
i_test_hole = ibset(0_bit_kind,j_hole)
if(iand(key_in(k_hole,ispin2),i_test_hole).ne.i_test_hole)then
i_ok = 0
return
endif
key_out(k_hole,ispin2) = ibclr(key_out(k_hole,ispin2),j_hole)
k_particl = ishft(l-1,-bit_kind_shift)+1
j_particl = l-ishft(k_particl-1,bit_kind_shift)-1
i_test_particl = ibset(0_bit_kind,j_particl)
if(iand(key_in(k_particl,ispin2),i_test_particl).ne.0_bit_kind)then
i_ok = 0
return
endif
key_out(k_particl,ispin2) = ibset(key_out(k_particl,ispin2),j_particl)
i_ok = 1
end

51
src/Full_CI/parameters.irp.f Normal file
View File

@ -0,0 +1,51 @@
BEGIN_PROVIDER [ integer, N_det_max_fci ]
implicit none
BEGIN_DOC
! Max number od determinants in the wave function
END_DOC
logical :: exists
PROVIDE ezfio_filename
call ezfio_has_full_ci_n_det_max_fci(exists)
if (exists) then
call ezfio_get_full_ci_n_det_max_fci(n_det_max_fci)
else
n_det_max_fci = 10000
endif
call write_int(output_full_ci,n_det_max_fci,'Max number of determinants ')
ASSERT (n_det_max_fci > 0)
END_PROVIDER
BEGIN_PROVIDER [ logical , do_pt2_end ]
implicit none
BEGIN_DOC
! if True then compute the PT2 when the selection process is finished
END_DOC
logical :: exists
PROVIDE ezfio_filename
call ezfio_has_full_ci_do_pt2_end(exists)
if (exists) then
call ezfio_get_full_ci_do_pt2_end(do_pt2_end)
else
do_pt2_end = .True.
endif
!call write_i(output_full_ci,do_pt2_end,' computes the PT2 at the end of the selection ')
ASSERT (do_pt2_end > 0)
END_PROVIDER
BEGIN_PROVIDER [ double precision , pt2_max ]
implicit none
BEGIN_DOC
! The selection process stops when the largest PT2 (for all the states) is lower than pt2_max
! in absolute value
END_DOC
logical :: exists
PROVIDE ezfio_filename
call ezfio_has_full_ci_pt2_max(exists)
if (exists) then
call ezfio_get_full_ci_pt2_max(pt2_max)
else
pt2_max = 0.1d0
endif
END_PROVIDER

3
src/Hartree_Fock/Fock_matrix.irp.f
View File

@ -115,6 +115,7 @@ END_PROVIDER
if (do_direct_integrals) then
PROVIDE all_utils ao_overlap_abs ao_integrals_threshold
PROVIDE HF_density_matrix_ao_alpha HF_density_matrix_ao_beta
PROVIDE ao_bi_elec_integral_alpha
!$OMP PARALLEL DEFAULT(NONE) &
!$OMP PRIVATE(i,j,l,k1,k,integral) &
!$OMP SHARED(ao_num,ao_bi_elec_integral_alpha,ao_mono_elec_integral,&
@ -147,6 +148,8 @@ END_PROVIDER
!$OMP END PARALLEL
else
PROVIDE ao_bielec_integrals_in_map
!$OMP PARALLEL DEFAULT(NONE) &
!$OMP PRIVATE(i,j,l,k1,k,integral,ao_ints_val,ao_ints_idx,kmax) &
!$OMP SHARED(ao_num,ao_bi_elec_integral_alpha,ao_mono_elec_integral,&