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Provide mo...in_map -> all_mo_integrals

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This commit is contained in:
Anthony Scemama 2025-01-20 18:03:19 +01:00
parent 09f6d338e8
commit 348f606791
29 changed files with 574 additions and 573 deletions
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28
src/casscf_cipsi/bielec.irp.f
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@ -1,7 +1,7 @@
BEGIN_PROVIDER [real*8, bielec_PQxx_array, (mo_num, mo_num,n_core_inact_act_orb,n_core_inact_act_orb)]
BEGIN_DOC
! WARNING !!! Old version !!! NOT USED ANYMORE IN THE PROGRAM !!! TOO BIG TO BE STORED ON LARGE SYSTEMS !!!
!
! WARNING !!! Old version !!! NOT USED ANYMORE IN THE PROGRAM !!! TOO BIG TO BE STORED ON LARGE SYSTEMS !!!
!
! Replaced by the Cholesky-based function bielec_PQxx
!
! bielec_PQxx_array : integral (pq|xx) with p,q arbitrary, x core or active
@ -13,10 +13,10 @@ BEGIN_PROVIDER [real*8, bielec_PQxx_array, (mo_num, mo_num,n_core_inact_act_orb,
print*,''
print*,'Providing bielec_PQxx_array, WARNING IT CAN BE A VERY BIG ARRAY WHEN MO_NUM IS LARGE !!!'
print*,''
bielec_PQxx_array(:,:,:,:) = 0.d0
PROVIDE mo_two_e_integrals_in_map
PROVIDE all_mo_integrals
!$OMP PARALLEL DEFAULT(NONE) &
!$OMP PRIVATE(i,ii,j,jj,i3,j3) &
!$OMP SHARED(n_core_inact_orb,list_core_inact,mo_num,bielec_PQxx_array, &
@ -61,8 +61,8 @@ END_PROVIDER
BEGIN_PROVIDER [real*8, bielec_PxxQ_array, (mo_num,n_core_inact_act_orb,n_core_inact_act_orb, mo_num)]
BEGIN_DOC
! WARNING !!! Old version !!! NOT USED ANYMORE IN THE PROGRAM !!! TOO BIG TO BE STORED ON LARGE SYSTEMS !!!
!
! WARNING !!! Old version !!! NOT USED ANYMORE IN THE PROGRAM !!! TOO BIG TO BE STORED ON LARGE SYSTEMS !!!
!
! Replaced by the Cholesky-based function bielec_PxxQ
!
! bielec_PxxQ_array : integral (px|xq) with p,q arbitrary, x core or active
@ -72,11 +72,11 @@ BEGIN_PROVIDER [real*8, bielec_PxxQ_array, (mo_num,n_core_inact_act_orb,n_core_i
integer :: i,j,ii,jj,p,q,i3,j3,t3,v3
double precision, allocatable :: integrals_array(:,:)
real*8 :: mo_two_e_integral
print*,''
print*,'Providing bielec_PxxQ_array, WARNING IT CAN BE A VERY BIG ARRAY WHEN MO_NUM IS LARGE !!!'
print*,''
PROVIDE mo_two_e_integrals_in_map
PROVIDE all_mo_integrals
bielec_PxxQ_array = 0.d0
!$OMP PARALLEL DEFAULT(NONE) &
@ -85,7 +85,7 @@ BEGIN_PROVIDER [real*8, bielec_PxxQ_array, (mo_num,n_core_inact_act_orb,n_core_i
!$OMP n_act_orb,mo_integrals_map,list_act)
allocate(integrals_array(mo_num,mo_num))
!$OMP DO
do i=1,n_core_inact_orb
ii=list_core_inact(i)
@ -143,17 +143,17 @@ BEGIN_PROVIDER [real*8, bielecCI, (n_act_orb,n_act_orb,n_act_orb, mo_num)]
BEGIN_DOC
! bielecCI : integrals (tu|vp) with p arbitrary, tuv active
! index p runs over the whole basis, t,u,v only over the active orbitals
!
!
! This array can be stored anyway. Ex: 50 active orbitals, 1500 MOs ==> 8x50^3x1500 = 1.5 Gb
END_DOC
implicit none
integer :: i,j,k,p,t,u,v
double precision, external :: mo_two_e_integral
double precision :: wall0, wall1
double precision :: wall0, wall1
call wall_time(wall0)
print*,'Providing bielecCI'
PROVIDE mo_two_e_integrals_in_map
PROVIDE all_mo_integrals
!$OMP PARALLEL DO DEFAULT(NONE) &
!$OMP PRIVATE(i,j,k,p,t,u,v) &
!$OMP SHARED(mo_num,n_act_orb,list_act,bielecCI)

2
src/casscf_cipsi/hessian.irp.f
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@ -380,7 +380,7 @@ BEGIN_PROVIDER [double precision, hessmat, (nMonoEx,nMonoEx)]
! c-v | X X
! a-v | X
provide mo_two_e_integrals_in_map
provide all_mo_integrals
hessmat = 0.d0

52
src/casscf_cipsi/hessian_old.irp.f
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@ -13,18 +13,18 @@ BEGIN_PROVIDER [real*8, hessmat_old, (nMonoEx,nMonoEx)]
integer :: jndx,jhole,jpart
character*3 :: iexc,jexc
real*8 :: res
if (bavard) then
write(6,*) ' providing Hessian matrix hessmat_old '
write(6,*) ' nMonoEx = ',nMonoEx
endif
do indx=1,nMonoEx
do jndx=1,nMonoEx
hessmat_old(indx,jndx)=0.D0
end do
end do
do indx=1,nMonoEx
ihole=excit(1,indx)
ipart=excit(2,indx)
@ -38,7 +38,7 @@ BEGIN_PROVIDER [real*8, hessmat_old, (nMonoEx,nMonoEx)]
hessmat_old(jndx,indx)=res
end do
end do
END_PROVIDER
subroutine calc_hess_elem(ihole,ipart,jhole,jpart,res)
@ -75,9 +75,9 @@ subroutine calc_hess_elem(ihole,ipart,jhole,jpart,res)
integer :: nu_rs_possible
integer :: mu_pqrs_possible
integer :: mu_rspq_possible
res=0.D0
! the terms <0|E E H |0>
do mu=1,n_det
! get the string of the determinant
@ -174,10 +174,10 @@ subroutine calc_hess_elem(ihole,ipart,jhole,jpart,res)
end if
end do
end do
! state-averaged Hessian
res*=1.D0/dble(N_states)
end subroutine calc_hess_elem
BEGIN_PROVIDER [real*8, hessmat_peter, (nMonoEx,nMonoEx)]
@ -190,26 +190,26 @@ BEGIN_PROVIDER [real*8, hessmat_peter, (nMonoEx,nMonoEx)]
END_DOC
implicit none
integer :: i,j,t,u,a,b,indx,jndx,bstart,ustart,indx_shift
real*8 :: hessmat_itju
real*8 :: hessmat_itja
real*8 :: hessmat_itua
real*8 :: hessmat_iajb
real*8 :: hessmat_iatb
real*8 :: hessmat_taub
if (bavard) then
write(6,*) ' providing Hessian matrix hessmat_peter '
write(6,*) ' nMonoEx = ',nMonoEx
endif
provide mo_two_e_integrals_in_map
provide all_mo_integrals
!$OMP PARALLEL DEFAULT(NONE) &
!$OMP SHARED(hessmat_peter,n_core_inact_orb,n_act_orb,n_virt_orb,nMonoEx) &
!$OMP PRIVATE(i,indx,jndx,j,ustart,t,u,a,bstart,indx_shift)
!$OMP DO
! (DOUBLY OCCUPIED ---> ACT )
! (DOUBLY OCCUPIED ---> ACT )
do i=1,n_core_inact_orb
do t=1,n_act_orb
indx = t + (i-1)*n_act_orb
@ -226,14 +226,14 @@ BEGIN_PROVIDER [real*8, hessmat_peter, (nMonoEx,nMonoEx)]
jndx+=1
end do
end do
! (DOUBLY OCCUPIED ---> VIRTUAL)
! (DOUBLY OCCUPIED ---> VIRTUAL)
do j=1,n_core_inact_orb
do a=1,n_virt_orb
hessmat_peter(jndx,indx)=hessmat_itja(i,t,j,a)
jndx+=1
end do
end do
! (ACTIVE ---> VIRTUAL)
! (ACTIVE ---> VIRTUAL)
do u=1,n_act_orb
do a=1,n_virt_orb
hessmat_peter(jndx,indx)=hessmat_itua(i,t,u,a)
@ -243,15 +243,15 @@ BEGIN_PROVIDER [real*8, hessmat_peter, (nMonoEx,nMonoEx)]
end do
end do
!$OMP END DO NOWAIT
indx_shift = n_core_inact_orb*n_act_orb
!$OMP DO
! (DOUBLY OCCUPIED ---> VIRTUAL)
! (DOUBLY OCCUPIED ---> VIRTUAL)
do a=1,n_virt_orb
do i=1,n_core_inact_orb
indx = a + (i-1)*n_virt_orb + indx_shift
jndx=indx
! (DOUBLY OCCUPIED ---> VIRTUAL)
! (DOUBLY OCCUPIED ---> VIRTUAL)
do j=i,n_core_inact_orb
if (i.eq.j) then
bstart=a
@ -263,7 +263,7 @@ BEGIN_PROVIDER [real*8, hessmat_peter, (nMonoEx,nMonoEx)]
jndx+=1
end do
end do
! (ACT ---> VIRTUAL)
! (ACT ---> VIRTUAL)
do t=1,n_act_orb
do b=1,n_virt_orb
hessmat_peter(jndx,indx)=hessmat_iatb(i,a,t,b)
@ -273,15 +273,15 @@ BEGIN_PROVIDER [real*8, hessmat_peter, (nMonoEx,nMonoEx)]
end do
end do
!$OMP END DO NOWAIT
indx_shift += n_core_inact_orb*n_virt_orb
!$OMP DO
! (ACT ---> VIRTUAL)
!$OMP DO
! (ACT ---> VIRTUAL)
do a=1,n_virt_orb
do t=1,n_act_orb
indx = a + (t-1)*n_virt_orb + indx_shift
jndx=indx
! (ACT ---> VIRTUAL)
! (ACT ---> VIRTUAL)
do u=t,n_act_orb
if (t.eq.u) then
bstart=a
@ -295,16 +295,16 @@ BEGIN_PROVIDER [real*8, hessmat_peter, (nMonoEx,nMonoEx)]
end do
end do
end do
!$OMP END DO
!$OMP END DO
!$OMP END PARALLEL
do jndx=1,nMonoEx
do indx=1,jndx-1
hessmat_peter(indx,jndx) = hessmat_peter(jndx,indx)
enddo
enddo
END_PROVIDER

2
src/ccsd/ccsd_space_orb_sub.irp.f
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@ -35,7 +35,7 @@ subroutine run_ccsd_space_orb
PROVIDE cholesky_mo_transp
FREE cholesky_ao
else
PROVIDE mo_two_e_integrals_in_map
PROVIDE all_mo_integrals
endif
det = psi_det(:,:,cc_ref)

6
src/cipsi/stochastic_cipsi.irp.f
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@ -1,11 +1,11 @@
subroutine run_stochastic_cipsi(Ev,PT2)
subroutine run_stochastic_cipsi(Ev,PT2)
use selection_types
implicit none
BEGIN_DOC
! Selected Full Configuration Interaction with Stochastic selection and PT2.
END_DOC
integer :: i,j,k
double precision, intent(out) :: Ev(N_states), PT2(N_states)
double precision, intent(out) :: Ev(N_states), PT2(N_states)
double precision, allocatable :: zeros(:)
integer :: to_select
type(pt2_type) :: pt2_data, pt2_data_err
@ -14,7 +14,7 @@ subroutine run_stochastic_cipsi(Ev,PT2)
double precision :: rss
double precision, external :: memory_of_double
PROVIDE H_apply_buffer_allocated distributed_davidson mo_two_e_integrals_in_map
PROVIDE H_apply_buffer_allocated distributed_davidson all_mo_integrals
threshold_generators = 1.d0
SOFT_TOUCH threshold_generators

2
src/cipsi_utils/pt2_stoch_routines.irp.f
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@ -165,7 +165,7 @@ subroutine ZMQ_pt2(E, pt2_data, pt2_data_err, relative_error, N_in)
state_average_weight(pt2_stoch_istate) = 1.d0
TOUCH state_average_weight pt2_stoch_istate selection_weight
PROVIDE nproc pt2_F mo_two_e_integrals_in_map mo_one_e_integrals pt2_w
PROVIDE nproc pt2_F all_mo_integrals mo_one_e_integrals pt2_w
PROVIDE psi_selectors pt2_u pt2_J pt2_R
call new_parallel_job(zmq_to_qp_run_socket, zmq_socket_pull, 'pt2')

2
src/cipsi_utils/slave_cipsi.irp.f
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@ -14,7 +14,7 @@ subroutine run_slave_cipsi
end
subroutine provide_everything
PROVIDE H_apply_buffer_allocated mo_two_e_integrals_in_map psi_det_generators psi_coef_generators psi_det_sorted_bit psi_selectors n_det_generators n_states generators_bitmask zmq_context N_states_diag
PROVIDE H_apply_buffer_allocated all_mo_integrals psi_det_generators psi_coef_generators psi_det_sorted_bit psi_selectors n_det_generators n_states generators_bitmask zmq_context N_states_diag
PROVIDE pt2_e0_denominator mo_num N_int ci_energy mpi_master zmq_state zmq_context
PROVIDE psi_det psi_coef threshold_generators state_average_weight
PROVIDE N_det_selectors pt2_stoch_istate N_det selection_weight pseudo_sym

2
src/dressing/dress_slave.irp.f
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@ -15,7 +15,7 @@ subroutine dress_slave
end
subroutine provide_everything
PROVIDE H_apply_buffer_allocated mo_two_e_integrals_in_map psi_det_generators psi_coef_generators psi_det_sorted_bit psi_selectors n_det_generators n_states generators_bitmask zmq_context
PROVIDE H_apply_buffer_allocated all_mo_integrals psi_det_generators psi_coef_generators psi_det_sorted_bit psi_selectors n_det_generators n_states generators_bitmask zmq_context
end
subroutine run_wf

2
src/dressing/dress_stoch_routines.irp.f
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@ -258,7 +258,7 @@ subroutine ZMQ_dress(E, dress, delta_out, delta_s2_out, relative_error)
state_average_weight(dress_stoch_istate) = 1.d0
TOUCH state_average_weight dress_stoch_istate
provide nproc mo_two_e_integrals_in_map mo_one_e_integrals psi_selectors pt2_F pt2_N_teeth dress_M_m
provide nproc all_mo_integrals mo_one_e_integrals psi_selectors pt2_F pt2_N_teeth dress_M_m
print *, '========== ================= ================= ================='
print *, ' Samples Energy Stat. Error Seconds '

5
src/fci/fci.irp.f
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@ -36,8 +36,9 @@ program fci
!
END_DOC
PROVIDE all_mo_integrals
if (.not.is_zmq_slave) then
PROVIDE psi_det psi_coef mo_two_e_integrals_in_map
PROVIDE psi_det psi_coef
write(json_unit,json_array_open_fmt) 'fci'
@ -55,7 +56,7 @@ program fci
call json_close
else
PROVIDE mo_two_e_integrals_in_map pt2_min_parallel_tasks
PROVIDE pt2_min_parallel_tasks
call run_slave_cipsi

16
src/fci/pt2.irp.f
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@ -11,7 +11,7 @@ program pt2
!
! The main option for the |PT2| correction is the
! :option:`perturbation pt2_relative_error` which is the relative
! stochastic error on the |PT2| to reach before stopping the
! stochastic error on the |PT2| to reach before stopping the
! sampling.
!
END_DOC
@ -19,7 +19,7 @@ program pt2
read_wf = .True.
threshold_generators = 1.d0
SOFT_TOUCH read_wf threshold_generators
PROVIDE mo_two_e_integrals_in_map
PROVIDE all_mo_integrals
PROVIDE psi_energy
call run
else
@ -32,22 +32,22 @@ subroutine run
use selection_types
integer :: i,j,k
logical, external :: detEq
type(pt2_type) :: pt2_data, pt2_data_err
integer :: degree
integer :: n_det_before, to_select
double precision :: threshold_davidson_in
double precision :: relative_error
double precision, allocatable :: E_CI_before(:)
allocate ( E_CI_before(N_states))
call pt2_alloc(pt2_data, N_states)
call pt2_alloc(pt2_data_err, N_states)
E_CI_before(:) = psi_energy(:) + nuclear_repulsion
relative_error=PT2_relative_error
if (do_pt2) then
call ZMQ_pt2(psi_energy_with_nucl_rep, pt2_data, pt2_data_err, relative_error, 0) ! Stochastic PT2
else
@ -56,7 +56,7 @@ subroutine run
call print_summary(psi_energy_with_nucl_rep(1:N_states), &
pt2_data, pt2_data_err, N_det,N_configuration,N_states,psi_s2)
call save_energy(E_CI_before, pt2_data % pt2)
call pt2_dealloc(pt2_data)
call pt2_dealloc(pt2_data_err)

22
src/mo_optimization/debug_gradient_list_opt.irp.f
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@ -19,7 +19,7 @@
program debug_gradient_list
implicit none
! Variables
@ -30,12 +30,12 @@ program debug_gradient_list
double precision :: threshold
double precision :: max_error, max_elem, norm
integer :: nb_error
m = dim_list_act_orb
! Definition of n
! Definition of n
n = m*(m-1)/2
PROVIDE mo_two_e_integrals_in_map ! Verifier pour suppression
PROVIDE all_mo_integrals ! Verifier pour suppression
! Allocation
allocate(v_grad(n), v_grad2(n))
@ -44,15 +44,15 @@ program debug_gradient_list
call diagonalize_ci ! Verifier pour suppression
! Gradient
! Gradient
call gradient_list_opt(n,m,list_act,v_grad,max_elem,norm)
call first_gradient_list_opt(n,m,list_act,v_grad2)
v_grad = v_grad - v_grad2
nb_error = 0
max_error = 0d0
threshold = 1d-12
max_error = 0d0
threshold = 1d-12
do i = 1, n
if (ABS(v_grad(i)) > threshold) then
@ -65,9 +65,9 @@ program debug_gradient_list
endif
enddo
print*,''
print*,'Check the gradient'
print*,'Check the gradient'
print*,'Threshold:', threshold
print*,'Nb error:', nb_error
print*,'Max error:', max_error

22
src/mo_optimization/debug_gradient_opt.irp.f
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@ -19,7 +19,7 @@
program debug_gradient
implicit none
! Variables
@ -30,27 +30,27 @@ program debug_gradient
double precision :: threshold
double precision :: max_error, max_elem
integer :: nb_error
! Definition of n
! Definition of n
n = mo_num*(mo_num-1)/2
PROVIDE mo_two_e_integrals_in_map ! Check for suppression
PROVIDE all_mo_integrals ! Check for suppression
! Allocation
allocate(v_grad(n), v_grad2(n))
! Calculation
call diagonalize_ci
call diagonalize_ci
! Gradient
! Gradient
call first_gradient_opt(n,v_grad)
call gradient_opt(n,v_grad2,max_elem)
v_grad = v_grad - v_grad2
nb_error = 0
max_error = 0d0
threshold = 1d-12
max_error = 0d0
threshold = 1d-12
do i = 1, n
if (ABS(v_grad(i)) > threshold) then
@ -63,9 +63,9 @@ program debug_gradient
endif
enddo
print*,''
print*,'Check the gradient'
print*,'Check the gradient'
print*,'Threshold :', threshold
print*,'Nb error :', nb_error
print*,'Max error :', max_error

32
src/mo_optimization/debug_hessian_list_opt.irp.f
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@ -43,18 +43,18 @@ program debug_hessian_list_opt
double precision :: max_error, max_error_H
integer :: nb_error, nb_error_H
double precision :: threshold
m = dim_list_act_orb !mo_num
! Definition of n
! Definition of n
n = m*(m-1)/2
PROVIDE mo_two_e_integrals_in_map
PROVIDE all_mo_integrals
! Hessian
! Hessian
if (optimization_method == 'full') then
print*,'Use the full hessian matrix'
allocate(H(n,n),H2(n,n))
allocate(H(n,n),H2(n,n))
allocate(h_f(m,m,m,m),h_f2(m,m,m,m))
call hessian_list_opt(n,m,list_act,H,h_f)
@ -65,7 +65,7 @@ program debug_hessian_list_opt
h_f = h_f - h_f2
H = H - H2
max_error = 0d0
nb_error = 0
nb_error = 0
threshold = 1d-12
do l = 1, m
@ -99,7 +99,7 @@ program debug_hessian_list_opt
endif
enddo
enddo
enddo
! Deallocation
deallocate(H, H2, h_f, h_f2)
@ -110,26 +110,26 @@ program debug_hessian_list_opt
allocate(H(n,1),H2(n,1))
call diag_hessian_list_opt(n,m,list_act,H)
call first_diag_hessian_list_opt(n,m,list_act,H2)
H = H - H2
max_error_H = 0d0
nb_error_H = 0
do i = 1, n
if (ABS(H(i,1)) > threshold) then
print*, H(i,1)
nb_error_H = nb_error_H + 1
if (ABS(H(i,1)) > ABS(max_error_H)) then
max_error_H = H(i,1)
endif
endif
enddo
endif
print*,''
if (optimization_method == 'full') then
print*,'Check of the full hessian'
@ -140,8 +140,8 @@ program debug_hessian_list_opt
else
print*,'Check of the diagonal hessian'
endif
print*,'Nb error_H:', nb_error_H
print*,'Max error_H:', max_error_H
end program

34
src/mo_optimization/debug_hessian_opt.irp.f
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@ -36,20 +36,20 @@ program debug_hessian
double precision :: max_error, max_error_H
integer :: nb_error, nb_error_H
double precision :: threshold
! Definition of n
! Definition of n
n = mo_num*(mo_num-1)/2
PROVIDE mo_two_e_integrals_in_map
PROVIDE all_mo_integrals
! Allocation
allocate(H(n,n),H2(n,n))
allocate(H(n,n),H2(n,n))
allocate(h_f(mo_num,mo_num,mo_num,mo_num),h_f2(mo_num,mo_num,mo_num,mo_num))
! Calculation
! Hessian
if (optimization_method == 'full') then
! Hessian
if (optimization_method == 'full') then
print*,'Use the full hessian matrix'
call hessian_opt(n,H,h_f)
@ -59,7 +59,7 @@ program debug_hessian
h_f = h_f - h_f2
H = H - H2
max_error = 0d0
nb_error = 0
nb_error = 0
threshold = 1d-12
do l = 1, mo_num
@ -93,7 +93,7 @@ program debug_hessian
endif
enddo
enddo
enddo
elseif (optimization_method == 'diag') then
@ -128,43 +128,43 @@ program debug_hessian
enddo
h=H-H2
max_error_H = 0d0
nb_error_H = 0
do j = 1, n
do i = 1, n
if (ABS(H(i,j)) > threshold) then
print*, H(i,j)
nb_error_H = nb_error_H + 1
if (ABS(H(i,j)) > ABS(max_error_H)) then
max_error_H = H(i,j)
endif
endif
enddo
enddo
else
print*,'Unknown optimization_method, please select full, diag'
call abort
endif
print*,''
if (optimization_method == 'full') then
print*,'Check the full hessian'
else
print*,'Check the diagonal hessian'
endif
print*,'Threshold :', threshold
print*,'Nb error :', nb_error
print*,'Max error :', max_error
print*,''
print*,'Nb error_H :', nb_error_H
print*,'Max error_H :', max_error_H
! Deallocation
deallocate(H,H2,h_f,h_f2)

6
src/mo_optimization_utils/routine_opt_mos.irp.f
View File

@ -9,7 +9,7 @@ subroutine run_optimization_mos_CIPSI
logical :: not_converged
character (len=100) :: filename
PROVIDE psi_det psi_coef mo_two_e_integrals_in_map ao_pseudo_integrals
PROVIDE psi_det psi_coef all_mo_integrals ao_pseudo_integrals
allocate(Ev(N_states),PT2(N_states))
not_converged = .True.
@ -30,7 +30,7 @@ subroutine run_optimization_mos_CIPSI
print*,'======================'
print*,' Cipsi step:', nb_iter
print*,'======================'
print*,''
print*,''
print*,'********** cipsi step **********'
! cispi calculation
call run_stochastic_cipsi(Ev,PT2)
@ -70,7 +70,7 @@ subroutine run_optimization_mos_CIPSI
print*, 'The program will exit'
exit
endif
! To double the number of determinants in the wf
N_det_max = int(dble(n_det * 2)*0.9)
TOUCH N_det_max

38
src/mo_optimization_utils/run_orb_opt_trust_v2.irp.f
View File

@ -93,7 +93,7 @@ subroutine run_orb_opt_trust_v2
integer,allocatable :: tmp_list(:), key(:)
double precision, allocatable :: tmp_m_x(:,:),tmp_R(:,:), tmp_x(:), W(:,:), e_val(:)
PROVIDE mo_two_e_integrals_in_map ci_energy psi_det psi_coef
PROVIDE all_mo_integrals ci_energy psi_det psi_coef
! Allocation
@ -110,17 +110,17 @@ allocate(tmp_R(m,m), tmp_m_x(m,m), tmp_x(tmp_n))
allocate(e_val(tmp_n),key(tmp_n),v_grad(tmp_n))
! Method
! There are three different methods :
! There are three different methods :
! - the "full" hessian, which uses all the elements of the hessian
! matrix"
! - the "diagonal" hessian, which uses only the diagonal elements of the
! hessian
! - without the hessian (hessian = identity matrix)
! - without the hessian (hessian = identity matrix)
!Display the method
print*, 'Method :', optimization_method
if (optimization_method == 'full') then
if (optimization_method == 'full') then
print*, 'Full hessian'
allocate(H(tmp_n,tmp_n), h_f(m,m,m,m),W(tmp_n,tmp_n))
tmp_n2 = tmp_n
@ -147,13 +147,13 @@ print*, 'Absolute value of the hessian:', absolute_eig
! - We diagonalize the hessian
! - We compute a step and loop to reduce the radius of the
! trust region (and the size of the step by the way) until the step is
! accepted
! - We repeat the process until the convergence
! accepted
! - We repeat the process until the convergence
! NB: the convergence criterion can be changed
! Loop until the convergence of the optimization
! call diagonalize_ci
! call diagonalize_ci
!### Initialization ###
nb_iter = 0
@ -183,14 +183,14 @@ do while (not_converged)
! Full hessian
call hessian_list_opt(tmp_n, m, tmp_list, H, h_f)
! Diagonalization of the hessian
! Diagonalization of the hessian
call diagonalization_hessian(tmp_n, H, e_val, w)
elseif (optimization_method == 'diag') then
! Diagonal hessian
! Diagonal hessian
call diag_hessian_list_opt(tmp_n, m, tmp_list, H)
else
! Identity matrix
! Identity matrix
do tmp_i = 1, tmp_n
H(tmp_i,1) = 1d0
enddo
@ -212,7 +212,7 @@ do while (not_converged)
endif
! Init before the internal loop
cancel_step = .True. ! To enter in the loop just after
cancel_step = .True. ! To enter in the loop just after
nb_cancel = 0
nb_sub_iter = 0
@ -225,15 +225,15 @@ do while (not_converged)
print*,'Max elem grad:', max_elem_grad
print*,'-----------------------------'
! Hessian,gradient,Criterion -> x
call trust_region_step_w_expected_e(tmp_n,tmp_n2,H,W,e_val,v_grad,prev_criterion,rho,nb_iter,delta,criterion_model,tmp_x,must_exit)
! Hessian,gradient,Criterion -> x
call trust_region_step_w_expected_e(tmp_n,tmp_n2,H,W,e_val,v_grad,prev_criterion,rho,nb_iter,delta,criterion_model,tmp_x,must_exit)
if (must_exit) then
print*,'step_in_trust_region sends: Exit'
exit
endif
! 1D tmp -> 2D tmp
! 1D tmp -> 2D tmp
call vec_to_mat_v2(tmp_n, m, tmp_x, tmp_m_x)
! Rotation matrix for the active MOs
@ -250,14 +250,14 @@ do while (not_converged)
call sub_to_full_rotation_matrix(m, tmp_list, tmp_R, R)
! MO rotations
call apply_mo_rotation(R, prev_mos)
call apply_mo_rotation(R, prev_mos)
! Update of the energy before the diagonalization of the hamiltonian
call clear_mo_map
TOUCH mo_coef psi_det psi_coef ci_energy two_e_dm_mo
TOUCH mo_coef psi_det psi_coef ci_energy two_e_dm_mo
call state_average_energy(criterion)
! Criterion -> step accepted or rejected
! Criterion -> step accepted or rejected
call trust_region_is_step_cancelled(nb_iter, prev_criterion, criterion, criterion_model, rho, cancel_step)
! Cancellation of the step if necessary
@ -283,7 +283,7 @@ do while (not_converged)
! To exit the external loop if must_exit = .True.
if (must_exit) then
exit
endif
endif
! Step accepted, nb iteration + 1
nb_iter = nb_iter + 1
@ -295,7 +295,7 @@ do while (not_converged)
endif
if (nb_iter >= optimization_max_nb_iter) then
print*,'Not converged: nb_iter >= optimization_max_nb_iter'
not_converged = .False.
not_converged = .False.
endif
if (.not. not_converged) then

2
src/mo_two_e_ints/map_integrals.irp.f
View File

@ -6,7 +6,7 @@ BEGIN_PROVIDER [ logical, all_mo_integrals ]
! Used to provide everything needed before using MO integrals
! PROVIDE all_mo_integrals
END_DOC
PROVIDE mo_two_e_integrals_in_map mo_integrals_cache mo_two_e_integrals_jj_exchange mo_two_e_integrals_jj_anti mo_two_e_integrals_jj big_array_exchange_integrals big_array_coulomb_integrals
PROVIDE mo_two_e_integrals_in_map mo_integrals_cache mo_two_e_integrals_jj_exchange mo_two_e_integrals_jj_anti mo_two_e_integrals_jj big_array_exchange_integrals big_array_coulomb_integrals mo_one_e_integrals
END_PROVIDER

80
src/mu_of_r/f_hf_utils.irp.f
View File

@ -1,41 +1,41 @@
BEGIN_PROVIDER [double precision, two_e_int_hf_f, (n_basis_orb,n_basis_orb,n_max_occ_val_orb_for_hf,n_max_occ_val_orb_for_hf)]
implicit none
BEGIN_DOC
! list of two-electron integrals (built with the MOs belonging to the \mathcal{B} space)
!
! needed to compute the function f_{HF}(r_1,r_2)
! list of two-electron integrals (built with the MOs belonging to the \mathcal{B} space)
!
! needed to compute the function f_{HF}(r_1,r_2)
!
! two_e_int_hf_f(j,i,n,m) = < j i | n m > where all orbitals belong to "list_basis"
END_DOC
integer :: orb_i,orb_j,i,j,orb_m,orb_n,m,n
double precision :: get_two_e_integral
PROVIDE mo_two_e_integrals_in_map mo_integrals_map big_array_exchange_integrals
do orb_m = 1, n_max_occ_val_orb_for_hf! electron 1
PROVIDE all_mo_integrals big_array_exchange_integrals
do orb_m = 1, n_max_occ_val_orb_for_hf! electron 1
m = list_valence_orb_for_hf(orb_m,1)
do orb_n = 1, n_max_occ_val_orb_for_hf! electron 2
do orb_n = 1, n_max_occ_val_orb_for_hf! electron 2
n = list_valence_orb_for_hf(orb_n,1)
do orb_i = 1, n_basis_orb ! electron 1
do orb_i = 1, n_basis_orb ! electron 1
i = list_basis(orb_i)
do orb_j = 1, n_basis_orb ! electron 2
do orb_j = 1, n_basis_orb ! electron 2
j = list_basis(orb_j)
! 2 1 2 1
two_e_int_hf_f(orb_j,orb_i,orb_n,orb_m) = get_two_e_integral(m,n,i,j,mo_integrals_map)
two_e_int_hf_f(orb_j,orb_i,orb_n,orb_m) = get_two_e_integral(m,n,i,j,mo_integrals_map)
enddo
enddo
enddo
enddo
END_PROVIDER
END_PROVIDER
subroutine f_HF_valence_ab(r1,r2,f_HF_val_ab,two_bod_dens)
implicit none
BEGIN_DOC
! f_HF_val_ab(r1,r2) = function f_{\Psi^B}(X_1,X_2) of Eq. (22) of J. Chem. Phys. 149, 194301 (2018)
!
! for alpha beta spins and an HF wave function and excluding the "core" orbitals (see Eq. 16a of Phys.Chem.Lett.2019, 10, 2931 2937)
!
! two_bod_dens = on-top pair density of the HF wave function
! f_HF_val_ab(r1,r2) = function f_{\Psi^B}(X_1,X_2) of Eq. (22) of J. Chem. Phys. 149, 194301 (2018)
!
! < HF | wee_{\alpha\beta} | HF > = \int (r1,r2) f_HF_ab(r1,r2) excluding all contributions from "core" "electrons"
! for alpha beta spins and an HF wave function and excluding the "core" orbitals (see Eq. 16a of Phys.Chem.Lett.2019, 10, 2931 2937)
!
! two_bod_dens = on-top pair density of the HF wave function
!
! < HF | wee_{\alpha\beta} | HF > = \int (r1,r2) f_HF_ab(r1,r2) excluding all contributions from "core" "electrons"
END_DOC
double precision, intent(in) :: r1(3), r2(3)
double precision, intent(out):: f_HF_val_ab,two_bod_dens
@ -50,8 +50,8 @@ subroutine f_HF_valence_ab(r1,r2,f_HF_val_ab,two_bod_dens)
allocate(mos_array_valence_r1(n_basis_orb) , mos_array_valence_r2(n_basis_orb), mos_array_r1(mo_num), mos_array_r2(mo_num))
allocate(mos_array_valence_hf_r1(n_occ_val_orb_for_hf(1)) , mos_array_valence_hf_r2(n_occ_val_orb_for_hf(2)) )
! You get all orbitals in r_1 and r_2
call give_all_mos_at_r(r1,mos_array_r1)
call give_all_mos_at_r(r2,mos_array_r2)
call give_all_mos_at_r(r1,mos_array_r1)
call give_all_mos_at_r(r2,mos_array_r2)
! You extract the occupied ALPHA/BETA orbitals belonging to the space \mathcal{A}
do i_m = 1, n_occ_val_orb_for_hf(1)
mos_array_valence_hf_r1(i_m) = mos_array_r1(list_valence_orb_for_hf(i_m,1))
@ -61,7 +61,7 @@ subroutine f_HF_valence_ab(r1,r2,f_HF_val_ab,two_bod_dens)
enddo
! You extract the orbitals belonging to the space \mathcal{B}
do i_m = 1, n_basis_orb
do i_m = 1, n_basis_orb
mos_array_valence_r1(i_m) = mos_array_r1(list_basis(i_m))
mos_array_valence_r2(i_m) = mos_array_r2(list_basis(i_m))
enddo
@ -70,24 +70,24 @@ subroutine f_HF_valence_ab(r1,r2,f_HF_val_ab,two_bod_dens)
f_HF_val_ab = 0.d0
two_bod_dens = 0.d0
! You browse all OCCUPIED ALPHA electrons in the \mathcal{A} space
do m = 1, n_occ_val_orb_for_hf(1)! electron 1
do m = 1, n_occ_val_orb_for_hf(1)! electron 1
! You browse all OCCUPIED BETA electrons in the \mathcal{A} space
do n = 1, n_occ_val_orb_for_hf(2)! electron 2
do n = 1, n_occ_val_orb_for_hf(2)! electron 2
! two_bod_dens(r_1,r_2) = n_alpha(r_1) * n_beta(r_2)
two_bod_dens += mos_array_valence_hf_r1(m) * mos_array_valence_hf_r1(m) * mos_array_valence_hf_r2(n) * mos_array_valence_hf_r2(n)
! You browse all COUPLE OF ORBITALS in the \mathacal{B} space
two_bod_dens += mos_array_valence_hf_r1(m) * mos_array_valence_hf_r1(m) * mos_array_valence_hf_r2(n) * mos_array_valence_hf_r2(n)
! You browse all COUPLE OF ORBITALS in the \mathacal{B} space
do i = 1, n_basis_orb
do j = 1, n_basis_orb
! 2 1 2 1
f_HF_val_ab += two_e_int_hf_f(j,i,n,m) &
* mos_array_valence_r1(i) * mos_array_valence_hf_r1(m) &
* mos_array_valence_r2(j) * mos_array_valence_hf_r2(n)
f_HF_val_ab += two_e_int_hf_f(j,i,n,m) &
* mos_array_valence_r1(i) * mos_array_valence_hf_r1(m) &
* mos_array_valence_r2(j) * mos_array_valence_hf_r2(n)
enddo
enddo
enddo
enddo
! multiply by two to adapt to the N(N-1) normalization condition of the active two-rdm
f_HF_val_ab *= 2.d0
f_HF_val_ab *= 2.d0
two_bod_dens *= 2.d0
end
@ -95,14 +95,14 @@ end
subroutine integral_f_HF_valence_ab(r1,int_f_HF_val_ab)
implicit none
BEGIN_DOC
! in_f_HF_val_ab(r_1) = \int dr_2 f_{\Psi^B}(r_1,r_2)
!
! where f_{\Psi^B}(r_1,r_2) is defined by Eq. (22) of J. Chem. Phys. 149, 194301 (2018)
! in_f_HF_val_ab(r_1) = \int dr_2 f_{\Psi^B}(r_1,r_2)
!
! where f_{\Psi^B}(r_1,r_2) is defined by Eq. (22) of J. Chem. Phys. 149, 194301 (2018)
!
! for alpha beta spins and an HF wave function and excluding the "core" orbitals (see Eq. 16a of Phys.Chem.Lett.2019, 10, 2931 2937)
!
! Such function can be used to test if the f_HF_val_ab(r_1,r_2) is correctly built.
!
! Such function can be used to test if the f_HF_val_ab(r_1,r_2) is correctly built.
!
! < HF | wee_{\alpha\beta} | HF > = \int (r1) int_f_HF_val_ab(r_1)
END_DOC
double precision, intent(in) :: r1(3)
@ -114,28 +114,28 @@ subroutine integral_f_HF_valence_ab(r1,int_f_HF_val_ab)
double precision, allocatable :: mos_array_valence_r1(:)
double precision, allocatable :: mos_array_valence_hf_r1(:)
double precision :: get_two_e_integral
call give_all_mos_at_r(r1,mos_array_r1)
call give_all_mos_at_r(r1,mos_array_r1)
allocate(mos_array_valence_r1( n_basis_orb ))
allocate(mos_array_valence_hf_r1( n_occ_val_orb_for_hf(1) ) )
do i_m = 1, n_occ_val_orb_for_hf(1)
mos_array_valence_hf_r1(i_m) = mos_array_r1(list_valence_orb_for_hf(i_m,1))
enddo
do i_m = 1, n_basis_orb
do i_m = 1, n_basis_orb
mos_array_valence_r1(i_m) = mos_array_r1(list_basis(i_m))
enddo
int_f_HF_val_ab = 0.d0
! You browse all OCCUPIED ALPHA electrons in the \mathcal{A} space
do m = 1, n_occ_val_orb_for_hf(1)! electron 1
do m = 1, n_occ_val_orb_for_hf(1)! electron 1
! You browse all OCCUPIED BETA electrons in the \mathcal{A} space
do n = 1, n_occ_val_orb_for_hf(2)! electron 2
! You browse all ORBITALS in the \mathacal{B} space
do n = 1, n_occ_val_orb_for_hf(2)! electron 2
! You browse all ORBITALS in the \mathacal{B} space
do i = 1, n_basis_orb
! due to integration in real-space and the use of orthonormal MOs, a Kronecker delta_jn shoes up
! due to integration in real-space and the use of orthonormal MOs, a Kronecker delta_jn shoes up
j = n
! 2 1 2 1
int_f_HF_val_ab += two_e_int_hf_f(j,i,n,m) &
* mos_array_valence_r1(i) * mos_array_valence_hf_r1(m)
int_f_HF_val_ab += two_e_int_hf_f(j,i,n,m) &
* mos_array_valence_r1(i) * mos_array_valence_hf_r1(m)
enddo
enddo
enddo

144
src/mu_of_r/f_psi_i_a_v_utils.irp.f
View File

@ -1,7 +1,7 @@
subroutine give_f_ii_val_ab(r1,r2,f_ii_val_ab,two_bod_dens)
implicit none
BEGIN_DOC
! contribution from purely inactive orbitals to f_{\Psi^B}(r_1,r_2) for a CAS wave function
! contribution from purely inactive orbitals to f_{\Psi^B}(r_1,r_2) for a CAS wave function
END_DOC
double precision, intent(in) :: r1(3),r2(3)
double precision, intent(out):: f_ii_val_ab,two_bod_dens
@ -9,13 +9,13 @@ subroutine give_f_ii_val_ab(r1,r2,f_ii_val_ab,two_bod_dens)
integer :: i_i,i_j
double precision, allocatable :: mos_array_inact_r1(:),mos_array_inact_r2(:)
double precision, allocatable :: mos_array_basis_r1(:),mos_array_basis_r2(:)
double precision, allocatable :: mos_array_r1(:) , mos_array_r2(:)
double precision, allocatable :: mos_array_r1(:) , mos_array_r2(:)
double precision :: get_two_e_integral
! You get all orbitals in r_1 and r_2
allocate(mos_array_r1(mo_num) , mos_array_r2(mo_num) )
call give_all_mos_at_r(r1,mos_array_r1)
call give_all_mos_at_r(r2,mos_array_r2)
! You extract the inactive orbitals
call give_all_mos_at_r(r1,mos_array_r1)
call give_all_mos_at_r(r2,mos_array_r2)
! You extract the inactive orbitals
allocate(mos_array_inact_r1(n_inact_orb) , mos_array_inact_r2(n_inact_orb) )
do i_m = 1, n_inact_orb
mos_array_inact_r1(i_m) = mos_array_r1(list_inact(i_m))
@ -26,7 +26,7 @@ subroutine give_f_ii_val_ab(r1,r2,f_ii_val_ab,two_bod_dens)
! You extract the orbitals belonging to the space \mathcal{B}
allocate(mos_array_basis_r1(n_basis_orb) , mos_array_basis_r2(n_basis_orb) )
do i_m = 1, n_basis_orb
do i_m = 1, n_basis_orb
mos_array_basis_r1(i_m) = mos_array_r1(list_basis(i_m))
mos_array_basis_r2(i_m) = mos_array_r2(list_basis(i_m))
enddo
@ -34,30 +34,30 @@ subroutine give_f_ii_val_ab(r1,r2,f_ii_val_ab,two_bod_dens)
f_ii_val_ab = 0.d0
two_bod_dens = 0.d0
! You browse all OCCUPIED ALPHA electrons in the \mathcal{A} space
do m = 1, n_inact_orb ! electron 1
do m = 1, n_inact_orb ! electron 1
! You browse all OCCUPIED BETA electrons in the \mathcal{A} space
do n = 1, n_inact_orb ! electron 2
do n = 1, n_inact_orb ! electron 2
! two_bod_dens(r_1,r_2) = n_alpha(r_1) * n_beta(r_2)
two_bod_dens += mos_array_inact_r1(m) * mos_array_inact_r1(m) * mos_array_inact_r2(n) * mos_array_inact_r2(n)
! You browse all COUPLE OF ORBITALS in the \mathacal{B} space
two_bod_dens += mos_array_inact_r1(m) * mos_array_inact_r1(m) * mos_array_inact_r2(n) * mos_array_inact_r2(n)
! You browse all COUPLE OF ORBITALS in the \mathacal{B} space
do i = 1, n_basis_orb
do j = 1, n_basis_orb
! 2 1 2 1
f_ii_val_ab += two_e_int_ii_f(j,i,n,m) * mos_array_inact_r1(m) * mos_array_basis_r1(i) &
* mos_array_inact_r2(n) * mos_array_basis_r2(j)
f_ii_val_ab += two_e_int_ii_f(j,i,n,m) * mos_array_inact_r1(m) * mos_array_basis_r1(i) &
* mos_array_inact_r2(n) * mos_array_basis_r2(j)
enddo
enddo
enddo
enddo
! multiply by two to adapt to the N(N-1) normalization condition of the active two-rdm
f_ii_val_ab *= 2.d0
f_ii_val_ab *= 2.d0
two_bod_dens *= 2.d0
end
subroutine give_f_ia_val_ab(r1,r2,f_ia_val_ab,two_bod_dens,istate)
BEGIN_DOC
! contribution from inactive and active orbitals to f_{\Psi^B}(r_1,r_2) for the "istate" state of a CAS wave function
! contribution from inactive and active orbitals to f_{\Psi^B}(r_1,r_2) for the "istate" state of a CAS wave function
END_DOC
implicit none
integer, intent(in) :: istate
@ -65,7 +65,7 @@ subroutine give_f_ia_val_ab(r1,r2,f_ia_val_ab,two_bod_dens,istate)
double precision, intent(out):: f_ia_val_ab,two_bod_dens
integer :: i,orb_i,a,orb_a,n,m,b
double precision :: rho
double precision, allocatable :: mos_array_r1(:) , mos_array_r2(:)
double precision, allocatable :: mos_array_r1(:) , mos_array_r2(:)
double precision, allocatable :: mos_array_inact_r1(:),mos_array_inact_r2(:)
double precision, allocatable :: mos_array_basis_r1(:),mos_array_basis_r2(:)
double precision, allocatable :: mos_array_act_r1(:),mos_array_act_r2(:)
@ -75,10 +75,10 @@ subroutine give_f_ia_val_ab(r1,r2,f_ia_val_ab,two_bod_dens,istate)
two_bod_dens = 0.d0
! You get all orbitals in r_1 and r_2
allocate(mos_array_r1(mo_num) , mos_array_r2(mo_num) )
call give_all_mos_at_r(r1,mos_array_r1)
call give_all_mos_at_r(r2,mos_array_r2)
call give_all_mos_at_r(r1,mos_array_r1)
call give_all_mos_at_r(r2,mos_array_r2)
! You extract the inactive orbitals
! You extract the inactive orbitals
allocate( mos_array_inact_r1(n_inact_orb) , mos_array_inact_r2(n_inact_orb) )
do i = 1, n_inact_orb
mos_array_inact_r1(i) = mos_array_r1(list_inact(i))
@ -87,7 +87,7 @@ subroutine give_f_ia_val_ab(r1,r2,f_ia_val_ab,two_bod_dens,istate)
mos_array_inact_r2(i) = mos_array_r2(list_inact(i))
enddo
! You extract the active orbitals
! You extract the active orbitals
allocate( mos_array_act_r1(n_basis_orb) , mos_array_act_r2(n_basis_orb) )
do i= 1, n_act_orb
mos_array_act_r1(i) = mos_array_r1(list_act(i))
@ -109,11 +109,11 @@ subroutine give_f_ia_val_ab(r1,r2,f_ia_val_ab,two_bod_dens,istate)
! rho_tilde(i,a) = \sum_b rho(b,a) * phi_i(1) * phi_j(2)
allocate(rho_tilde(n_inact_orb,n_act_orb))
two_bod_dens = 0.d0
do a = 1, n_act_orb
do a = 1, n_act_orb
do i = 1, n_inact_orb
rho_tilde(i,a) = 0.d0
do b = 1, n_act_orb
rho = one_e_act_dm_beta_mo_for_dft(b,a,istate) + one_e_act_dm_alpha_mo_for_dft(b,a,istate)
do b = 1, n_act_orb
rho = one_e_act_dm_beta_mo_for_dft(b,a,istate) + one_e_act_dm_alpha_mo_for_dft(b,a,istate)
two_bod_dens += mos_array_inact_r1(i) * mos_array_inact_r1(i) * mos_array_act_r2(a) * mos_array_act_r2(b) * rho
rho_tilde(i,a) += rho * mos_array_inact_r1(i) * mos_array_act_r2(b)
enddo
@ -125,12 +125,12 @@ subroutine give_f_ia_val_ab(r1,r2,f_ia_val_ab,two_bod_dens,istate)
allocate( v_tilde(n_act_orb,n_act_orb) )
allocate( integrals_array(mo_num,mo_num) )
v_tilde = 0.d0
do a = 1, n_act_orb
do a = 1, n_act_orb
orb_a = list_act(a)
do i = 1, n_inact_orb
v_tilde(i,a) = 0.d0
orb_i = list_inact(i)
! call get_mo_two_e_integrals_ij(orb_i,orb_a,mo_num,integrals_array,mo_integrals_map)
! call get_mo_two_e_integrals_ij(orb_i,orb_a,mo_num,integrals_array,mo_integrals_map)
do m = 1, n_basis_orb
do n = 1, n_basis_orb
! v_tilde(i,a) += integrals_array(n,m) * mos_array_basis_r2(n) * mos_array_basis_r1(m)
@ -146,14 +146,14 @@ subroutine give_f_ia_val_ab(r1,r2,f_ia_val_ab,two_bod_dens,istate)
enddo
enddo
! multiply by two to adapt to the N(N-1) normalization condition of the active two-rdm
f_ia_val_ab *= 2.d0
f_ia_val_ab *= 2.d0
two_bod_dens *= 2.d0
end
subroutine give_f_aa_val_ab(r1,r2,f_aa_val_ab,two_bod_dens,istate)
BEGIN_DOC
! contribution from purely active orbitals to f_{\Psi^B}(r_1,r_2) for the "istate" state of a CAS wave function
! contribution from purely active orbitals to f_{\Psi^B}(r_1,r_2) for the "istate" state of a CAS wave function
END_DOC
implicit none
integer, intent(in) :: istate
@ -161,7 +161,7 @@ subroutine give_f_aa_val_ab(r1,r2,f_aa_val_ab,two_bod_dens,istate)
double precision, intent(out):: f_aa_val_ab,two_bod_dens
integer :: i,orb_i,a,orb_a,n,m,b,c,d
double precision :: rho
double precision, allocatable :: mos_array_r1(:) , mos_array_r2(:)
double precision, allocatable :: mos_array_r1(:) , mos_array_r2(:)
double precision, allocatable :: mos_array_basis_r1(:),mos_array_basis_r2(:)
double precision, allocatable :: mos_array_act_r1(:),mos_array_act_r2(:)
double precision, allocatable :: integrals_array(:,:),rho_tilde(:,:),v_tilde(:,:)
@ -170,10 +170,10 @@ subroutine give_f_aa_val_ab(r1,r2,f_aa_val_ab,two_bod_dens,istate)
two_bod_dens = 0.d0
! You get all orbitals in r_1 and r_2
allocate(mos_array_r1(mo_num) , mos_array_r2(mo_num) )
call give_all_mos_at_r(r1,mos_array_r1)
call give_all_mos_at_r(r2,mos_array_r2)
call give_all_mos_at_r(r1,mos_array_r1)
call give_all_mos_at_r(r2,mos_array_r2)
! You extract the active orbitals
! You extract the active orbitals
allocate( mos_array_act_r1(n_basis_orb) , mos_array_act_r2(n_basis_orb) )
do i= 1, n_act_orb
mos_array_act_r1(i) = mos_array_r1(list_act(i))
@ -201,8 +201,8 @@ subroutine give_f_aa_val_ab(r1,r2,f_aa_val_ab,two_bod_dens,istate)
do c = 1, n_act_orb ! 1
do d = 1, n_act_orb ! 2
rho = mos_array_act_r1(c) * mos_array_act_r2(d) * act_2_rdm_ab_mo(d,c,b,a,istate)
rho_tilde(b,a) += rho
two_bod_dens += rho * mos_array_act_r1(a) * mos_array_act_r2(b)
rho_tilde(b,a) += rho
two_bod_dens += rho * mos_array_act_r1(a) * mos_array_act_r2(b)
enddo
enddo
enddo
@ -212,7 +212,7 @@ subroutine give_f_aa_val_ab(r1,r2,f_aa_val_ab,two_bod_dens,istate)
! v_tilde(i,a) = \sum_{m,n} phi_m(1) * phi_n(2) < i a | m n >
allocate( v_tilde(n_act_orb,n_act_orb) )
v_tilde = 0.d0
do a = 1, n_act_orb
do a = 1, n_act_orb
do b = 1, n_act_orb
v_tilde(b,a) = 0.d0
do m = 1, n_basis_orb
@ -235,92 +235,92 @@ end
BEGIN_PROVIDER [double precision, two_e_int_aa_f, (n_basis_orb,n_basis_orb,n_act_orb,n_act_orb)]
implicit none
BEGIN_DOC
! list of two-electron integrals (built with the MOs belonging to the \mathcal{B} space)
!
! needed to compute the function f_{ii}(r_1,r_2)
! list of two-electron integrals (built with the MOs belonging to the \mathcal{B} space)
!
! needed to compute the function f_{ii}(r_1,r_2)
!
! two_e_int_aa_f(j,i,n,m) = < j i | n m > where all orbitals belong to "list_basis"
END_DOC
integer :: orb_i,orb_j,i,j,orb_m,orb_n,m,n
double precision :: integrals_array(mo_num,mo_num),get_two_e_integral
PROVIDE mo_two_e_integrals_in_map mo_integrals_map big_array_exchange_integrals
do orb_m = 1, n_act_orb ! electron 1
PROVIDE all_mo_integrals
do orb_m = 1, n_act_orb ! electron 1
m = list_act(orb_m)
do orb_n = 1, n_act_orb ! electron 2
do orb_n = 1, n_act_orb ! electron 2
n = list_act(orb_n)
call get_mo_two_e_integrals_ij(m,n,mo_num,integrals_array,mo_integrals_map)
do orb_i = 1, n_basis_orb ! electron 1
call get_mo_two_e_integrals_ij(m,n,mo_num,integrals_array,mo_integrals_map)
do orb_i = 1, n_basis_orb ! electron 1
i = list_basis(orb_i)
do orb_j = 1, n_basis_orb ! electron 2
do orb_j = 1, n_basis_orb ! electron 2
j = list_basis(orb_j)
! 2 1 2 1
two_e_int_aa_f(orb_j,orb_i,orb_n,orb_m) = get_two_e_integral(m,n,i,j,mo_integrals_map)
! two_e_int_aa_f(orb_j,orb_i,orb_n,orb_m) = integrals_array(j,i)
two_e_int_aa_f(orb_j,orb_i,orb_n,orb_m) = get_two_e_integral(m,n,i,j,mo_integrals_map)
! two_e_int_aa_f(orb_j,orb_i,orb_n,orb_m) = integrals_array(j,i)
enddo
enddo
enddo
enddo
END_PROVIDER
END_PROVIDER
BEGIN_PROVIDER [double precision, two_e_int_ia_f, (n_basis_orb,n_basis_orb,n_inact_orb,n_act_orb)]
implicit none
BEGIN_DOC
! list of two-electron integrals (built with the MOs belonging to the \mathcal{B} space)
!
! needed to compute the function f_{ia}(r_1,r_2)
! list of two-electron integrals (built with the MOs belonging to the \mathcal{B} space)
!
! needed to compute the function f_{ia}(r_1,r_2)
!
! two_e_int_aa_f(j,i,n,m) = < j i | n m > where all orbitals belong to "list_basis"
END_DOC
integer :: orb_i,orb_j,i,j,orb_m,orb_n,m,n
double precision :: integrals_array(mo_num,mo_num),get_two_e_integral
PROVIDE mo_two_e_integrals_in_map mo_integrals_map big_array_exchange_integrals
do orb_m = 1, n_act_orb ! electron 1
PROVIDE all_mo_integrals
do orb_m = 1, n_act_orb ! electron 1
m = list_act(orb_m)
do orb_n = 1, n_inact_orb ! electron 2
do orb_n = 1, n_inact_orb ! electron 2
n = list_inact(orb_n)
call get_mo_two_e_integrals_ij(m,n,mo_num,integrals_array,mo_integrals_map)
do orb_i = 1, n_basis_orb ! electron 1
call get_mo_two_e_integrals_ij(m,n,mo_num,integrals_array,mo_integrals_map)
do orb_i = 1, n_basis_orb ! electron 1
i = list_basis(orb_i)
do orb_j = 1, n_basis_orb ! electron 2
do orb_j = 1, n_basis_orb ! electron 2
j = list_basis(orb_j)
! 2 1 2 1
! two_e_int_ia_f(orb_j,orb_i,orb_n,orb_m) = get_two_e_integral(m,n,i,j,mo_integrals_map)
two_e_int_ia_f(orb_j,orb_i,orb_n,orb_m) = integrals_array(j,i)
! two_e_int_ia_f(orb_j,orb_i,orb_n,orb_m) = get_two_e_integral(m,n,i,j,mo_integrals_map)
two_e_int_ia_f(orb_j,orb_i,orb_n,orb_m) = integrals_array(j,i)
enddo
enddo
enddo
enddo
END_PROVIDER
END_PROVIDER
BEGIN_PROVIDER [double precision, two_e_int_ii_f, (n_basis_orb,n_basis_orb,n_inact_orb,n_inact_orb)]
implicit none
BEGIN_DOC
! list of two-electron integrals (built with the MOs belonging to the \mathcal{B} space)
!
! needed to compute the function f_{ii}(r_1,r_2)
! list of two-electron integrals (built with the MOs belonging to the \mathcal{B} space)
!
! needed to compute the function f_{ii}(r_1,r_2)
!
! two_e_int_ii_f(j,i,n,m) = < j i | n m > where all orbitals belong to "list_basis"
END_DOC
integer :: orb_i,orb_j,i,j,orb_m,orb_n,m,n
double precision :: get_two_e_integral,integrals_array(mo_num,mo_num)
PROVIDE mo_two_e_integrals_in_map mo_integrals_map big_array_exchange_integrals
do orb_m = 1, n_inact_orb ! electron 1
PROVIDE all_mo_integrals
do orb_m = 1, n_inact_orb ! electron 1
m = list_inact(orb_m)
do orb_n = 1, n_inact_orb ! electron 2
do orb_n = 1, n_inact_orb ! electron 2
n = list_inact(orb_n)
call get_mo_two_e_integrals_ij(m,n,mo_num,integrals_array,mo_integrals_map)
do orb_i = 1, n_basis_orb ! electron 1
call get_mo_two_e_integrals_ij(m,n,mo_num,integrals_array,mo_integrals_map)
do orb_i = 1, n_basis_orb ! electron 1
i = list_basis(orb_i)
do orb_j = 1, n_basis_orb ! electron 2
do orb_j = 1, n_basis_orb ! electron 2
j = list_basis(orb_j)
! 2 1 2 1
! two_e_int_ii_f(orb_j,orb_i,orb_n,orb_m) = get_two_e_integral(m,n,i,j,mo_integrals_map)
two_e_int_ii_f(orb_j,orb_i,orb_n,orb_m) = integrals_array(j,i)
! two_e_int_ii_f(orb_j,orb_i,orb_n,orb_m) = get_two_e_integral(m,n,i,j,mo_integrals_map)
two_e_int_ii_f(orb_j,orb_i,orb_n,orb_m) = integrals_array(j,i)
enddo
enddo
enddo
enddo
END_PROVIDER
END_PROVIDER
subroutine give_mu_of_r_cas(r,istate,mu_of_r,f_psi,n2_psi)
@ -343,13 +343,13 @@ subroutine give_mu_of_r_cas(r,istate,mu_of_r,f_psi,n2_psi)
! active-active part of f_psi(r1,r2)
call give_f_aa_val_ab(r,r,f_aa_val_ab,two_bod_dens_aa,istate)
f_psi = f_ii_val_ab + f_ia_val_ab + f_aa_val_ab
f_psi = f_ii_val_ab + f_ia_val_ab + f_aa_val_ab
n2_psi = two_bod_dens_ii + two_bod_dens_ia + two_bod_dens_aa
if(n2_psi.le.1.d-12.or.f_psi.le.0.d0.or.f_psi * n2_psi.lt.0.d0)then
w_psi = 1.d+10
else
else
w_psi = f_psi / n2_psi
endif
mu_of_r = w_psi * sqpi * 0.5d0
end

82
src/mu_of_r/mu_of_r_conditions.irp.f
View File

@ -1,12 +1,12 @@
BEGIN_PROVIDER [double precision, mu_of_r_prov, (n_points_final_grid,N_states) ]
implicit none
implicit none
BEGIN_DOC
! general variable for mu(r)
! general variable for mu(r)
!
! corresponds to Eq. (37) of J. Chem. Phys. 149, 194301 (2018)
! corresponds to Eq. (37) of J. Chem. Phys. 149, 194301 (2018)
!
! !!!!!! WARNING !!!!!! if no_core_density == .True. then all contributions from the core orbitals
! !!!!!! WARNING !!!!!! if no_core_density == .True. then all contributions from the core orbitals
!
! in the two-body density matrix are excluded
END_DOC
@ -31,7 +31,7 @@
mu_of_r_prov(ipoint,istate) = mu_of_r_hf_sparse(ipoint)
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
mu_of_r_prov(ipoint,istate) = mu_of_r_psi_cas(ipoint,istate)
else
else
print*,'you requested the following mu_of_r_potential'
print*,mu_of_r_potential
print*,'which does not correspond to any of the options for such keyword'
@ -42,23 +42,23 @@
if (write_mu_of_r) then
print*,'Writing mu(r) on disk ...'
call ezfio_set_mu_of_r_io_mu_of_r('Read')
call ezfio_set_mu_of_r_mu_of_r_disk(mu_of_r_prov)
call ezfio_set_mu_of_r_io_mu_of_r('Read')
call ezfio_set_mu_of_r_mu_of_r_disk(mu_of_r_prov)
endif
call wall_time(wall1)
print*,'Time to provide mu_of_r = ',wall1-wall0
END_PROVIDER
END_PROVIDER
BEGIN_PROVIDER [double precision, mu_of_r_hf, (n_points_final_grid) ]
implicit none
implicit none
BEGIN_DOC
! mu(r) computed with a HF wave function (assumes that HF MOs are stored in the EZFIO)
!
! corresponds to Eq. (37) of J. Chem. Phys. 149, 194301 (2018) but for \Psi^B = HF^B
!
! !!!!!! WARNING !!!!!! if no_core_density == .True. then all contributions from the core orbitals
! !!!!!! WARNING !!!!!! if no_core_density == .True. then all contributions from the core orbitals
!
! in the two-body density matrix are excluded
END_DOC
@ -70,14 +70,14 @@
sqpi = dsqrt(dacos(-1.d0))
!$OMP PARALLEL DO &
!$OMP DEFAULT (NONE) &
!$OMP PRIVATE (ipoint,f_hf,on_top,w_hf) &
!$OMP ShARED (n_points_final_grid,mu_of_r_hf,f_hf_cholesky,on_top_hf_grid,sqpi)
!$OMP PRIVATE (ipoint,f_hf,on_top,w_hf) &
!$OMP ShARED (n_points_final_grid,mu_of_r_hf,f_hf_cholesky,on_top_hf_grid,sqpi)
do ipoint = 1, n_points_final_grid
f_hf = f_hf_cholesky(ipoint)
on_top = on_top_hf_grid(ipoint)
if(on_top.le.1.d-12.or.f_hf.le.0.d0.or.f_hf * on_top.lt.0.d0)then
w_hf = 1.d+10
else
else
w_hf = f_hf / on_top
endif
mu_of_r_hf(ipoint) = w_hf * sqpi * 0.5d0
@ -85,16 +85,16 @@
!$OMP END PARALLEL DO
call wall_time(wall1)
print*,'Time to provide mu_of_r_hf = ',wall1-wall0
END_PROVIDER
END_PROVIDER
BEGIN_PROVIDER [double precision, mu_of_r_hf_sparse, (n_points_final_grid) ]
implicit none
implicit none
BEGIN_DOC
! mu(r) computed with a HF wave function (assumes that HF MOs are stored in the EZFIO)
!
! corresponds to Eq. (37) of J. Chem. Phys. 149, 194301 (2018) but for \Psi^B = HF^B
!
! !!!!!! WARNING !!!!!! if no_core_density == .True. then all contributions from the core orbitals
! !!!!!! WARNING !!!!!! if no_core_density == .True. then all contributions from the core orbitals
!
! in the two-body density matrix are excluded
END_DOC
@ -106,14 +106,14 @@
PROVIDE f_hf_cholesky_sparse on_top_hf_grid
!$OMP PARALLEL DO &
!$OMP DEFAULT (NONE) &
!$OMP PRIVATE (ipoint,f_hf,on_top,w_hf) &
!$OMP ShARED (n_points_final_grid,mu_of_r_hf_sparse,f_hf_cholesky_sparse,on_top_hf_grid,sqpi)
!$OMP PRIVATE (ipoint,f_hf,on_top,w_hf) &
!$OMP ShARED (n_points_final_grid,mu_of_r_hf_sparse,f_hf_cholesky_sparse,on_top_hf_grid,sqpi)
do ipoint = 1, n_points_final_grid
f_hf = f_hf_cholesky_sparse(ipoint)
on_top = on_top_hf_grid(ipoint)
if(on_top.le.1.d-12.or.f_hf.le.0.d0.or.f_hf * on_top.lt.0.d0)then
w_hf = 1.d+10
else
else
w_hf = f_hf / on_top
endif
mu_of_r_hf_sparse(ipoint) = w_hf * sqpi * 0.5d0
@ -121,36 +121,36 @@
!$OMP END PARALLEL DO
call wall_time(wall1)
print*,'Time to provide mu_of_r_hf_sparse = ',wall1-wall0
END_PROVIDER
END_PROVIDER
BEGIN_PROVIDER [double precision, mu_of_r_hf_old, (n_points_final_grid) ]
implicit none
implicit none
BEGIN_DOC
! mu(r) computed with a HF wave function (assumes that HF MOs are stored in the EZFIO)
!
! corresponds to Eq. (37) of J. Chem. Phys. 149, 194301 (2018) but for \Psi^B = HF^B
!
! !!!!!! WARNING !!!!!! if no_core_density == .True. then all contributions from the core orbitals
! !!!!!! WARNING !!!!!! if no_core_density == .True. then all contributions from the core orbitals
!
! in the two-body density matrix are excluded
END_DOC
integer :: ipoint
double precision :: wall0,wall1,f_hf,on_top,w_hf,sqpi
PROVIDE mo_two_e_integrals_in_map mo_integrals_map big_array_exchange_integrals
PROVIDE all_mo_integrals
print*,'providing mu_of_r_hf_old ...'
call wall_time(wall0)
sqpi = dsqrt(dacos(-1.d0))
provide f_psi_hf_ab
provide f_psi_hf_ab
!$OMP PARALLEL DO &
!$OMP DEFAULT (NONE) &
!$OMP PRIVATE (ipoint,f_hf,on_top,w_hf) &
!$OMP ShARED (n_points_final_grid,mu_of_r_hf_old,f_psi_hf_ab,on_top_hf_mu_r,sqpi)
!$OMP PRIVATE (ipoint,f_hf,on_top,w_hf) &
!$OMP ShARED (n_points_final_grid,mu_of_r_hf_old,f_psi_hf_ab,on_top_hf_mu_r,sqpi)
do ipoint = 1, n_points_final_grid
f_hf = f_psi_hf_ab(ipoint)
on_top = on_top_hf_mu_r(ipoint)
if(on_top.le.1.d-12.or.f_hf.le.0.d0.or.f_hf * on_top.lt.0.d0)then
w_hf = 1.d+10
else
else
w_hf = f_hf / on_top
endif
mu_of_r_hf_old(ipoint) = w_hf * sqpi * 0.5d0
@ -158,17 +158,17 @@
!$OMP END PARALLEL DO
call wall_time(wall1)
print*,'Time to provide mu_of_r_hf_old = ',wall1-wall0
END_PROVIDER
END_PROVIDER
BEGIN_PROVIDER [double precision, mu_of_r_psi_cas, (n_points_final_grid,N_states) ]
implicit none
implicit none
BEGIN_DOC
! mu(r) computed with a wave function developped in an active space
!
! corresponds to Eq. (37) of J. Chem. Phys. 149, 194301 (2018)
! corresponds to Eq. (37) of J. Chem. Phys. 149, 194301 (2018)
!
! !!!!!! WARNING !!!!!! if no_core_density == .True. then all contributions from the core orbitals
! !!!!!! WARNING !!!!!! if no_core_density == .True. then all contributions from the core orbitals
!
! in the one- and two-body density matrix are excluded
END_DOC
@ -181,15 +181,15 @@
provide f_psi_cas_ab
!$OMP PARALLEL DO &
!$OMP DEFAULT (NONE) &
!$OMP PRIVATE (ipoint,f_psi,on_top,w_psi,istate) &
!$OMP SHARED (n_points_final_grid,mu_of_r_psi_cas,f_psi_cas_ab,on_top_cas_mu_r,sqpi,N_states)
!$OMP PRIVATE (ipoint,f_psi,on_top,w_psi,istate) &
!$OMP SHARED (n_points_final_grid,mu_of_r_psi_cas,f_psi_cas_ab,on_top_cas_mu_r,sqpi,N_states)
do istate = 1, N_states
do ipoint = 1, n_points_final_grid
f_psi = f_psi_cas_ab(ipoint,istate)
on_top = on_top_cas_mu_r(ipoint,istate)
f_psi = f_psi_cas_ab(ipoint,istate)
on_top = on_top_cas_mu_r(ipoint,istate)
if(on_top.le.1.d-12.or.f_psi.le.0.d0.or.f_psi * on_top.lt.0.d0)then
w_psi = 1.d+10
else
else
w_psi = f_psi / on_top
endif
mu_of_r_psi_cas(ipoint,istate) = w_psi * sqpi * 0.5d0
@ -198,15 +198,15 @@
!$OMP END PARALLEL DO
call wall_time(wall1)
print*,'Time to provide mu_of_r_psi_cas = ',wall1-wall0
END_PROVIDER
END_PROVIDER
BEGIN_PROVIDER [double precision, mu_average_prov, (N_states)]
implicit none
BEGIN_DOC
! average value of mu(r) weighted with the total one-e density and divided by the number of electrons
! average value of mu(r) weighted with the total one-e density and divided by the number of electrons
!
! !!!!!! WARNING !!!!!! if no_core_density == .True. then all contributions from the core orbitals
! !!!!!! WARNING !!!!!! if no_core_density == .True. then all contributions from the core orbitals
!
! in the one- and two-body density matrix are excluded
END_DOC
@ -216,12 +216,12 @@
do istate = 1, N_states
do ipoint = 1, n_points_final_grid
weight =final_weight_at_r_vector(ipoint)
density = one_e_dm_and_grad_alpha_in_r(4,ipoint,istate) &
density = one_e_dm_and_grad_alpha_in_r(4,ipoint,istate) &
+ one_e_dm_and_grad_beta_in_r(4,ipoint,istate)
if(mu_of_r_prov(ipoint,istate).gt.1.d+09)cycle
mu_average_prov(istate) += mu_of_r_prov(ipoint,istate) * weight * density
enddo
mu_average_prov(istate) = mu_average_prov(istate) / elec_num_grid_becke(istate)
enddo
END_PROVIDER
END_PROVIDER

2
src/tools/fcidump.irp.f
View File

@ -41,7 +41,7 @@ program fcidump
integer(key_kind), allocatable :: keys(:)
double precision, allocatable :: values(:)
integer(cache_map_size_kind) :: n_elements, n_elements_max
PROVIDE mo_two_e_integrals_in_map
PROVIDE all_mo_integrals
double precision :: get_two_e_integral, integral

2
src/tools/fcidump_pyscf.irp.f
View File

@ -41,7 +41,7 @@ program fcidump_pyscf
integer(key_kind), allocatable :: keys(:)
double precision, allocatable :: values(:)
integer(cache_map_size_kind) :: n_elements, n_elements_max
PROVIDE mo_two_e_integrals_in_map
PROVIDE all_mo_integrals
double precision :: get_two_e_integral, integral

2
src/tools/four_idx_transform.irp.f
View File

@ -18,6 +18,6 @@ program four_idx_transform
io_mo_two_e_integrals = 'Write'
SOFT_TOUCH io_mo_two_e_integrals
if (.true.) then
PROVIDE mo_two_e_integrals_in_map
PROVIDE all_mo_integrals
endif
end

2
src/trexio/export_trexio_routines.irp.f
View File

@ -505,7 +505,7 @@ subroutine export_trexio(update,full_path)
if (export_mo_two_e_ints) then
print *, 'MO two-e integrals'
PROVIDE mo_two_e_integrals_in_map
PROVIDE all_mo_integrals
double precision, external :: mo_two_e_integral

76
src/two_body_rdm/act_2_rdm.irp.f
View File

@ -4,34 +4,34 @@
BEGIN_DOC
! 12 12
! 1 2 1 2 == <ij|kl>
! act_2_rdm_ab_mo(i,j,k,l,istate) = STATE SPECIFIC physicist notation for 2RDM of alpha/beta+beta/alpha electrons
!
! act_2_rdm_ab_mo(i,j,k,l,istate) = STATE SPECIFIC physicist notation for 2RDM of alpha/beta+beta/alpha electrons
!
! <Psi_{istate}| a^{\dagger}_{i \alpha} a^{\dagger}_{j \beta} a_{l \beta} a_{k \alpha} |Psi_{istate}>
!
! + <Psi_{istate}| a^{\dagger}_{i \beta} a^{\dagger}_{j \alpha} a_{l \alpha} a_{k \beta} |Psi_{istate}>
!
! WHERE ALL ORBITALS (i,j,k,l) BELONGS TO AN ACTIVE SPACE DEFINED BY "list_act"
! WHERE ALL ORBITALS (i,j,k,l) BELONGS TO AN ACTIVE SPACE DEFINED BY "list_act"
!
! THE NORMALIZATION (i.e. sum of diagonal elements) IS SET TO N_{\alpha}^{act} * N_{\beta}^{act} * 2
!
! !!!!! WARNING !!!!! ALL SLATER DETERMINANTS IN PSI_DET MUST BELONG TO AN ACTIVE SPACE DEFINED BY "list_act"
! !!!!! WARNING !!!!! ALL SLATER DETERMINANTS IN PSI_DET MUST BELONG TO AN ACTIVE SPACE DEFINED BY "list_act"
!
END_DOC
END_DOC
integer :: ispin
double precision :: wall_1, wall_2
character*(128) :: name_file
character*(128) :: name_file
name_file = 'act_2_rdm_ab_mo'
! condition for alpha/beta spin
print*,''
print*,'Providing act_2_rdm_ab_mo '
ispin = 3
ispin = 3
act_2_rdm_ab_mo = 0.d0
provide mo_two_e_integrals_in_map
provide all_mo_integrals
call wall_time(wall_1)
if(read_two_body_rdm_ab)then
print*,'Reading act_2_rdm_ab_mo from disk ...'
call read_array_two_rdm(n_act_orb,N_states,act_2_rdm_ab_mo,name_file)
else
else
call orb_range_2_rdm_openmp(act_2_rdm_ab_mo,n_act_orb,n_act_orb,list_act,ispin,psi_coef,size(psi_coef,2),size(psi_coef,1))
endif
if(write_two_body_rdm_ab)then
@ -42,36 +42,36 @@
call wall_time(wall_2)
print*,'Wall time to provide act_2_rdm_ab_mo',wall_2 - wall_1
act_2_rdm_ab_mo *= 2.d0
END_PROVIDER
END_PROVIDER
BEGIN_PROVIDER [double precision, act_2_rdm_aa_mo, (n_act_orb,n_act_orb,n_act_orb,n_act_orb,N_states)]
implicit none
BEGIN_DOC
! act_2_rdm_aa_mo(i,j,k,l,istate) = STATE SPECIFIC physicist notation for 2RDM of ALPHA/ALPHA electrons
!
! act_2_rdm_aa_mo(i,j,k,l,istate) = STATE SPECIFIC physicist notation for 2RDM of ALPHA/ALPHA electrons
!
! <Psi_{istate}| a^{\dagger}_{i \alpha} a^{\dagger}_{j \alpha} a_{l \alpha} a_{k \alpha} |Psi_{istate}>
!
! WHERE ALL ORBITALS (i,j,k,l) BELONGS TO AN ACTIVE SPACE DEFINED BY "list_act"
! WHERE ALL ORBITALS (i,j,k,l) BELONGS TO AN ACTIVE SPACE DEFINED BY "list_act"
!
! THE NORMALIZATION (i.e. sum of diagonal elements) IS SET TO N_{\alpha}^{act} * (N_{\alpha}^{act} - 1)
!
! !!!!! WARNING !!!!! ALL SLATER DETERMINANTS IN PSI_DET MUST BELONG TO AN ACTIVE SPACE DEFINED BY "list_act"
END_DOC
! !!!!! WARNING !!!!! ALL SLATER DETERMINANTS IN PSI_DET MUST BELONG TO AN ACTIVE SPACE DEFINED BY "list_act"
END_DOC
integer :: ispin
double precision :: wall_1, wall_2
! condition for alpha/beta spin
print*,''
print*,'Providing act_2_rdm_aa_mo '
character*(128) :: name_file
character*(128) :: name_file
name_file = 'act_2_rdm_aa_mo'
ispin = 1
ispin = 1
act_2_rdm_aa_mo = 0.d0
call wall_time(wall_1)
if(read_two_body_rdm_aa)then
print*,'Reading act_2_rdm_aa_mo from disk ...'
call read_array_two_rdm(n_act_orb,N_states,act_2_rdm_aa_mo,name_file)
else
else
call orb_range_2_rdm_openmp(act_2_rdm_aa_mo,n_act_orb,n_act_orb,list_act,ispin,psi_coef,size(psi_coef,2),size(psi_coef,1))
endif
if(write_two_body_rdm_aa)then
@ -83,36 +83,36 @@
call wall_time(wall_2)
print*,'Wall time to provide act_2_rdm_aa_mo',wall_2 - wall_1
act_2_rdm_aa_mo *= 2.d0
END_PROVIDER
END_PROVIDER
BEGIN_PROVIDER [double precision, act_2_rdm_bb_mo, (n_act_orb,n_act_orb,n_act_orb,n_act_orb,N_states)]
implicit none
BEGIN_DOC
! act_2_rdm_bb_mo(i,j,k,l,istate) = STATE SPECIFIC physicist notation for 2RDM of BETA/BETA electrons
!
! act_2_rdm_bb_mo(i,j,k,l,istate) = STATE SPECIFIC physicist notation for 2RDM of BETA/BETA electrons
!
! <Psi_{istate}| a^{\dagger}_{i \beta} a^{\dagger}_{j \beta} a_{l \beta} a_{k \beta} |Psi_{istate}>
!
! WHERE ALL ORBITALS (i,j,k,l) BELONGS TO AN ACTIVE SPACE DEFINED BY "list_act"
! WHERE ALL ORBITALS (i,j,k,l) BELONGS TO AN ACTIVE SPACE DEFINED BY "list_act"
!
! THE NORMALIZATION (i.e. sum of diagonal elements) IS SET TO N_{\beta}^{act} * (N_{\beta}^{act} - 1)
!
! !!!!! WARNING !!!!! ALL SLATER DETERMINANTS IN PSI_DET MUST BELONG TO AN ACTIVE SPACE DEFINED BY "list_act"
END_DOC
! !!!!! WARNING !!!!! ALL SLATER DETERMINANTS IN PSI_DET MUST BELONG TO AN ACTIVE SPACE DEFINED BY "list_act"
END_DOC
integer :: ispin
double precision :: wall_1, wall_2
! condition for beta/beta spin
print*,''
print*,'Providing act_2_rdm_bb_mo '
character*(128) :: name_file
character*(128) :: name_file
name_file = 'act_2_rdm_bb_mo'
ispin = 2
ispin = 2
act_2_rdm_bb_mo = 0.d0
call wall_time(wall_1)
if(read_two_body_rdm_bb)then
print*,'Reading act_2_rdm_bb_mo from disk ...'
call read_array_two_rdm(n_act_orb,N_states,act_2_rdm_bb_mo,name_file)
else
else
call orb_range_2_rdm_openmp(act_2_rdm_bb_mo,n_act_orb,n_act_orb,list_act,ispin,psi_coef,size(psi_coef,2),size(psi_coef,1))
endif
if(write_two_body_rdm_bb)then
@ -124,35 +124,35 @@
call wall_time(wall_2)
print*,'Wall time to provide act_2_rdm_bb_mo',wall_2 - wall_1
act_2_rdm_bb_mo *= 2.d0
END_PROVIDER
END_PROVIDER
BEGIN_PROVIDER [double precision, act_2_rdm_spin_trace_mo, (n_act_orb,n_act_orb,n_act_orb,n_act_orb,N_states)]
implicit none
BEGIN_DOC
! act_2_rdm_spin_trace_mo(i,j,k,l,istate) = STATE SPECIFIC physicist notation for 2RDM
!
! act_2_rdm_spin_trace_mo(i,j,k,l,istate) = STATE SPECIFIC physicist notation for 2RDM
!
! \sum_{\sigma,\sigma'}<Psi_{istate}| a^{\dagger}_{i \sigma} a^{\dagger}_{j \sigma'} a_{l \sigma'} a_{k \sigma} |Psi_{istate}>
!
! WHERE ALL ORBITALS (i,j,k,l) BELONGS TO AN ACTIVE SPACE DEFINED BY "list_act"
! WHERE ALL ORBITALS (i,j,k,l) BELONGS TO AN ACTIVE SPACE DEFINED BY "list_act"
!
! THE NORMALIZATION (i.e. sum of diagonal elements) IS SET TO N_{elec}^{act} * (N_{elec}^{act} - 1)
!
! !!!!! WARNING !!!!! ALL SLATER DETERMINANTS IN PSI_DET MUST BELONG TO AN ACTIVE SPACE DEFINED BY "list_act"
END_DOC
! !!!!! WARNING !!!!! ALL SLATER DETERMINANTS IN PSI_DET MUST BELONG TO AN ACTIVE SPACE DEFINED BY "list_act"
END_DOC
integer :: ispin
double precision :: wall_1, wall_2
! condition for beta/beta spin
print*,''
print*,'Providing act_2_rdm_spin_trace_mo '
character*(128) :: name_file
character*(128) :: name_file
name_file = 'act_2_rdm_spin_trace_mo'
ispin = 4
ispin = 4
act_2_rdm_spin_trace_mo = 0.d0
call wall_time(wall_1)
if(read_two_body_rdm_spin_trace)then
print*,'Reading act_2_rdm_spin_trace_mo from disk ...'
call read_array_two_rdm(n_act_orb,N_states,act_2_rdm_spin_trace_mo,name_file)
else
else
call orb_range_2_rdm_openmp(act_2_rdm_spin_trace_mo,n_act_orb,n_act_orb,list_act,ispin,psi_coef,size(psi_coef,2),size(psi_coef,1))
endif
if(write_two_body_rdm_spin_trace)then
@ -164,4 +164,4 @@
act_2_rdm_spin_trace_mo *= 2.d0
call wall_time(wall_2)
print*,'Wall time to provide act_2_rdm_spin_trace_mo',wall_2 - wall_1
END_PROVIDER
END_PROVIDER

228
src/two_rdm_routines/davidson_like_2rdm.irp.f
View File

@ -2,9 +2,9 @@ subroutine orb_range_2_rdm_openmp(big_array,dim1,norb,list_orb,ispin,u_0,N_st,sz
use bitmasks
implicit none
BEGIN_DOC
! if ispin == 1 :: alpha/alpha 2rdm
! == 2 :: beta /beta 2rdm
! == 3 :: alpha/beta + beta/alpha 2rdm
! if ispin == 1 :: alpha/alpha 2rdm
! == 2 :: beta /beta 2rdm
! == 3 :: alpha/beta + beta/alpha 2rdm
! == 4 :: spin traced 2rdm :: aa + bb + ab + ba
!
! Assumes that the determinants are in psi_det
@ -19,7 +19,7 @@ subroutine orb_range_2_rdm_openmp(big_array,dim1,norb,list_orb,ispin,u_0,N_st,sz
integer :: k
double precision, allocatable :: u_t(:,:)
!DIR$ ATTRIBUTES ALIGN : $IRP_ALIGN :: u_t
PROVIDE mo_two_e_integrals_in_map
PROVIDE all_mo_integrals
allocate(u_t(N_st,N_det))
do k=1,N_st
call dset_order(u_0(1,k),psi_bilinear_matrix_order,N_det)
@ -30,14 +30,14 @@ subroutine orb_range_2_rdm_openmp(big_array,dim1,norb,list_orb,ispin,u_0,N_st,sz
u_t, &
size(u_t, 1), &
N_det, N_st)
call orb_range_2_rdm_openmp_work(big_array,dim1,norb,list_orb,ispin,u_t,N_st,sze,1,N_det,0,1)
deallocate(u_t)
do k=1,N_st
call dset_order(u_0(1,k),psi_bilinear_matrix_order_reverse,N_det)
enddo
end
subroutine orb_range_2_rdm_openmp_work(big_array,dim1,norb,list_orb,ispin,u_t,N_st,sze,istart,iend,ishift,istep)
@ -52,11 +52,11 @@ subroutine orb_range_2_rdm_openmp_work(big_array,dim1,norb,list_orb,ispin,u_t,N_
integer, intent(in) :: dim1,norb,list_orb(norb),ispin
double precision, intent(inout) :: big_array(dim1,dim1,dim1,dim1)
double precision, intent(in) :: u_t(N_st,N_det)
integer :: k
PROVIDE N_int
select case (N_int)
case (1)
call orb_range_2_rdm_openmp_work_1(big_array,dim1,norb,list_orb,ispin,u_t,N_st,sze,istart,iend,ishift,istep)
@ -70,9 +70,9 @@ subroutine orb_range_2_rdm_openmp_work(big_array,dim1,norb,list_orb,ispin,u_t,N_
call orb_range_2_rdm_openmp_work_N_int(big_array,dim1,norb,list_orb,ispin,u_t,N_st,sze,istart,iend,ishift,istep)
end select
end
BEGIN_TEMPLATE
subroutine orb_range_2_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb,ispin,u_t,N_st,sze,istart,iend,ishift,istep)
@ -81,9 +81,9 @@ subroutine orb_range_2_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb,ispin
implicit none
BEGIN_DOC
! Computes the two rdm for the N_st vectors |u_t>
! if ispin == 1 :: alpha/alpha 2rdm
! == 2 :: beta /beta 2rdm
! == 3 :: alpha/beta 2rdm
! if ispin == 1 :: alpha/alpha 2rdm
! == 2 :: beta /beta 2rdm
! == 3 :: alpha/beta 2rdm
! == 4 :: spin traced 2rdm :: aa + bb + 0.5 (ab + ba))
! The 2rdm will be computed only on the list of orbitals list_orb, which contains norb
! Default should be 1,N_det,0,1 for istart,iend,ishift,istep
@ -92,7 +92,7 @@ subroutine orb_range_2_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb,ispin
double precision, intent(in) :: u_t(N_st,N_det)
integer, intent(in) :: dim1,norb,list_orb(norb),ispin
double precision, intent(inout) :: big_array(dim1,dim1,dim1,dim1)
integer(omp_lock_kind) :: lock_2rdm
integer :: i,j,k,l
integer :: k_a, k_b, l_a, l_b
@ -116,7 +116,7 @@ subroutine orb_range_2_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb,ispin
integer, allocatable :: keys(:,:)
double precision, allocatable :: values(:,:)
integer :: nkeys,sze_buff
alpha_alpha = .False.
alpha_alpha = .False.
beta_beta = .False.
alpha_beta = .False.
spin_trace = .False.
@ -134,27 +134,27 @@ subroutine orb_range_2_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb,ispin
stop
endif
PROVIDE N_int
call list_to_bitstring( orb_bitmask, list_orb, norb, N_int)
sze_buff = 6 * norb + elec_alpha_num * elec_alpha_num * 60
list_orb_reverse = -1000
sze_buff = 6 * norb + elec_alpha_num * elec_alpha_num * 60
list_orb_reverse = -1000
do i = 1, norb
list_orb_reverse(list_orb(i)) = i
list_orb_reverse(list_orb(i)) = i
enddo
maxab = max(N_det_alpha_unique, N_det_beta_unique)+1
allocate(idx0(maxab))
do i=1,maxab
idx0(i) = i
enddo
call omp_init_lock(lock_2rdm)
! Prepare the array of all alpha single excitations
! -------------------------------------------------
PROVIDE N_int nthreads_davidson elec_alpha_num
PROVIDE N_int nthreads_davidson elec_alpha_num
!$OMP PARALLEL DEFAULT(NONE) NUM_THREADS(nthreads_davidson) &
!$OMP SHARED(psi_bilinear_matrix_rows, N_det,lock_2rdm,&
!$OMP psi_bilinear_matrix_columns, &
@ -166,7 +166,7 @@ subroutine orb_range_2_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb,ispin
!$OMP psi_bilinear_matrix_order_transp_reverse, &
!$OMP psi_bilinear_matrix_columns_loc, &
!$OMP psi_bilinear_matrix_transp_rows_loc,elec_alpha_num, &
!$OMP istart, iend, istep, irp_here,list_orb_reverse, n_states, dim1, &
!$OMP istart, iend, istep, irp_here,list_orb_reverse, n_states, dim1, &
!$OMP ishift, idx0, u_t, maxab, alpha_alpha,beta_beta,alpha_beta,spin_trace,ispin,big_array,sze_buff,orb_bitmask) &
!$OMP PRIVATE(krow, kcol, tmp_det, spindet, k_a, k_b, i,c_1, &
!$OMP lcol, lrow, l_a, l_b, &
@ -174,35 +174,35 @@ subroutine orb_range_2_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb,ispin
!$OMP tmp_det2, idx, l, kcol_prev, &
!$OMP singles_a, n_singles_a, singles_b, &
!$OMP n_singles_b, nkeys, keys, values)
! Alpha/Beta double excitations
! =============================
nkeys = 0
allocate( keys(4,sze_buff), values(n_st,sze_buff))
allocate( keys(4,sze_buff), values(n_st,sze_buff))
allocate( buffer($N_int,maxab), &
singles_a(maxab), &
singles_b(maxab), &
doubles(maxab), &
idx(maxab))
kcol_prev=-1
ASSERT (iend <= N_det)
ASSERT (istart > 0)
ASSERT (istep > 0)
!$OMP DO SCHEDULE(dynamic,64)
do k_a=istart+ishift,iend,istep
krow = psi_bilinear_matrix_rows(k_a)
ASSERT (krow <= N_det_alpha_unique)
kcol = psi_bilinear_matrix_columns(k_a)
ASSERT (kcol <= N_det_beta_unique)
tmp_det(1:$N_int,1) = psi_det_alpha_unique(1:$N_int, krow)
tmp_det(1:$N_int,2) = psi_det_beta_unique (1:$N_int, kcol)
if (kcol /= kcol_prev) then
call get_all_spin_singles_$N_int( &
psi_det_beta_unique, idx0, &
@ -210,58 +210,58 @@ subroutine orb_range_2_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb,ispin
singles_b, n_singles_b)
endif
kcol_prev = kcol
! Loop over singly excited beta columns
! -------------------------------------
do i=1,n_singles_b
lcol = singles_b(i)
tmp_det2(1:$N_int,2) = psi_det_beta_unique(1:$N_int, lcol)
l_a = psi_bilinear_matrix_columns_loc(lcol)
ASSERT (l_a <= N_det)
do j=1,psi_bilinear_matrix_columns_loc(lcol+1) - l_a
lrow = psi_bilinear_matrix_rows(l_a)
ASSERT (lrow <= N_det_alpha_unique)
buffer(1:$N_int,j) = psi_det_alpha_unique(1:$N_int, lrow)
ASSERT (l_a <= N_det)
idx(j) = l_a
l_a = l_a+1
enddo
j = j-1
call get_all_spin_singles_$N_int( &
buffer, idx, tmp_det(1,1), j, &
singles_a, n_singles_a )
! Loop over alpha singles
! -----------------------
if(alpha_beta.or.spin_trace)then
do k = 1,n_singles_a
l_a = singles_a(k)
ASSERT (l_a <= N_det)
lrow = psi_bilinear_matrix_rows(l_a)
ASSERT (lrow <= N_det_alpha_unique)
tmp_det2(1:$N_int,1) = psi_det_alpha_unique(1:$N_int, lrow)
! print*,'nkeys before = ',nkeys
do l= 1, N_states
c_1(l) = u_t(l,l_a) * u_t(l,k_a)
enddo
if(alpha_beta)then
! only ONE contribution
! only ONE contribution
if (nkeys+1 .ge. sze_buff) then
call update_keys_values_n_states(keys,values,nkeys,dim1,n_st,big_array,lock_2rdm)
nkeys = 0
endif
else if (spin_trace)then
! TWO contributions
! TWO contributions
if (nkeys+2 .ge. sze_buff) then
call update_keys_values_n_states(keys,values,nkeys,dim1,n_st,big_array,lock_2rdm)
nkeys = 0
@ -271,42 +271,42 @@ subroutine orb_range_2_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb,ispin
enddo
endif
call update_keys_values_n_states(keys,values,nkeys,dim1,n_st,big_array,lock_2rdm)
nkeys = 0
enddo
enddo
!$OMP END DO
!$OMP DO SCHEDULE(dynamic,64)
do k_a=istart+ishift,iend,istep
! Single and double alpha exitations
! ===================================
! Initial determinant is at k_a in alpha-major representation
! -----------------------------------------------------------------------
krow = psi_bilinear_matrix_rows(k_a)
ASSERT (krow <= N_det_alpha_unique)
kcol = psi_bilinear_matrix_columns(k_a)
ASSERT (kcol <= N_det_beta_unique)
tmp_det(1:$N_int,1) = psi_det_alpha_unique(1:$N_int, krow)
tmp_det(1:$N_int,2) = psi_det_beta_unique (1:$N_int, kcol)
! Initial determinant is at k_b in beta-major representation
! ----------------------------------------------------------------------
k_b = psi_bilinear_matrix_order_transp_reverse(k_a)
ASSERT (k_b <= N_det)
spindet(1:$N_int) = tmp_det(1:$N_int,1)
! Loop inside the beta column to gather all the connected alphas
lcol = psi_bilinear_matrix_columns(k_a)
l_a = psi_bilinear_matrix_columns_loc(lcol)
@ -316,28 +316,28 @@ subroutine orb_range_2_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb,ispin
if (lcol /= kcol) exit
lrow = psi_bilinear_matrix_rows(l_a)
ASSERT (lrow <= N_det_alpha_unique)
buffer(1:$N_int,i) = psi_det_alpha_unique(1:$N_int, lrow)
idx(i) = l_a
l_a = l_a+1
enddo
i = i-1
call get_all_spin_singles_and_doubles_$N_int( &
buffer, idx, spindet, i, &
singles_a, doubles, n_singles_a, n_doubles )
! Compute Hij for all alpha singles
! ----------------------------------
tmp_det2(1:$N_int,2) = psi_det_beta_unique (1:$N_int, kcol)
do i=1,n_singles_a
l_a = singles_a(i)
ASSERT (l_a <= N_det)
lrow = psi_bilinear_matrix_rows(l_a)
ASSERT (lrow <= N_det_alpha_unique)
tmp_det2(1:$N_int,1) = psi_det_alpha_unique(1:$N_int, lrow)
do l= 1, N_states
c_1(l) = u_t(l,l_a) * u_t(l,k_a)
@ -356,23 +356,23 @@ subroutine orb_range_2_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb,ispin
endif
call orb_range_off_diag_single_to_all_states_aa_dm_buffer(tmp_det,tmp_det2,c_1,N_st,orb_bitmask,list_orb_reverse,ispin,sze_buff,nkeys,keys,values)
endif
enddo
call update_keys_values_n_states(keys,values,nkeys,dim1,n_st,big_array,lock_2rdm)
nkeys = 0
! Compute Hij for all alpha doubles
! ----------------------------------
if(alpha_alpha.or.spin_trace)then
do i=1,n_doubles
l_a = doubles(i)
ASSERT (l_a <= N_det)
lrow = psi_bilinear_matrix_rows(l_a)
ASSERT (lrow <= N_det_alpha_unique)
do l= 1, N_states
c_1(l) = u_t(l,l_a) * u_t(l,k_a)
enddo
@ -385,29 +385,29 @@ subroutine orb_range_2_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb,ispin
endif
call update_keys_values_n_states(keys,values,nkeys,dim1,n_st,big_array,lock_2rdm)
nkeys = 0
! Single and double beta excitations
! ==================================
! Initial determinant is at k_a in alpha-major representation
! -----------------------------------------------------------------------
krow = psi_bilinear_matrix_rows(k_a)
kcol = psi_bilinear_matrix_columns(k_a)
tmp_det(1:$N_int,1) = psi_det_alpha_unique(1:$N_int, krow)
tmp_det(1:$N_int,2) = psi_det_beta_unique (1:$N_int, kcol)
spindet(1:$N_int) = tmp_det(1:$N_int,2)
! Initial determinant is at k_b in beta-major representation
! -----------------------------------------------------------------------
k_b = psi_bilinear_matrix_order_transp_reverse(k_a)
ASSERT (k_b <= N_det)
! Loop inside the alpha row to gather all the connected betas
lrow = psi_bilinear_matrix_transp_rows(k_b)
l_b = psi_bilinear_matrix_transp_rows_loc(lrow)
@ -417,28 +417,28 @@ subroutine orb_range_2_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb,ispin
if (lrow /= krow) exit
lcol = psi_bilinear_matrix_transp_columns(l_b)
ASSERT (lcol <= N_det_beta_unique)
buffer(1:$N_int,i) = psi_det_beta_unique(1:$N_int, lcol)
idx(i) = l_b
l_b = l_b+1
enddo
i = i-1
call get_all_spin_singles_and_doubles_$N_int( &
buffer, idx, spindet, i, &
singles_b, doubles, n_singles_b, n_doubles )
! Compute Hij for all beta singles
! ----------------------------------
tmp_det2(1:$N_int,1) = psi_det_alpha_unique(1:$N_int, krow)
do i=1,n_singles_b
l_b = singles_b(i)
ASSERT (l_b <= N_det)
lcol = psi_bilinear_matrix_transp_columns(l_b)
ASSERT (lcol <= N_det_beta_unique)
tmp_det2(1:$N_int,2) = psi_det_beta_unique (1:$N_int, lcol)
l_a = psi_bilinear_matrix_transp_order(l_b)
do l= 1, N_states
@ -461,18 +461,18 @@ subroutine orb_range_2_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb,ispin
enddo
call update_keys_values_n_states(keys,values,nkeys,dim1,n_st,big_array,lock_2rdm)
nkeys = 0
! Compute Hij for all beta doubles
! ----------------------------------
if(beta_beta.or.spin_trace)then
do i=1,n_doubles
l_b = doubles(i)
ASSERT (l_b <= N_det)
lcol = psi_bilinear_matrix_transp_columns(l_b)
ASSERT (lcol <= N_det_beta_unique)
l_a = psi_bilinear_matrix_transp_order(l_b)
do l= 1, N_states
c_1(l) = u_t(l,l_a) * u_t(l,k_a)
@ -484,59 +484,59 @@ subroutine orb_range_2_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb,ispin
call orb_range_off_diag_double_to_all_states_bb_dm_buffer(tmp_det(1,2),psi_det_beta_unique(1, lcol),c_1,N_st,list_orb_reverse,ispin,sze_buff,nkeys,keys,values)
! print*,'to do orb_range_off_diag_double_to_2_rdm_bb_dm_buffer'
ASSERT (l_a <= N_det)
enddo
endif
call update_keys_values_n_states(keys,values,nkeys,dim1,n_st,big_array,lock_2rdm)
nkeys = 0
! Diagonal contribution
! =====================
! Initial determinant is at k_a in alpha-major representation
! -----------------------------------------------------------------------
krow = psi_bilinear_matrix_rows(k_a)
ASSERT (krow <= N_det_alpha_unique)
kcol = psi_bilinear_matrix_columns(k_a)
ASSERT (kcol <= N_det_beta_unique)
tmp_det(1:$N_int,1) = psi_det_alpha_unique(1:$N_int, krow)
tmp_det(1:$N_int,2) = psi_det_beta_unique (1:$N_int, kcol)
double precision, external :: diag_wee_mat_elem, diag_S_mat_elem
double precision :: c_1(N_states)
do l = 1, N_states
c_1(l) = u_t(l,k_a) * u_t(l,k_a)
enddo
call update_keys_values_n_states(keys,values,nkeys,dim1,n_st,big_array,lock_2rdm)
nkeys = 0
call orb_range_diag_to_all_states_2_rdm_dm_buffer(tmp_det,c_1,N_states,orb_bitmask,list_orb_reverse,ispin,sze_buff,nkeys,keys,values)
call update_keys_values_n_states(keys,values,nkeys,dim1,n_st,big_array,lock_2rdm)
nkeys = 0
end do
!$OMP END DO
deallocate(buffer, singles_a, singles_b, doubles, idx, keys, values)
!$OMP END PARALLEL
end
SUBST [ N_int ]
1;;
2;;
3;;
4;;
N_int;;
END_TEMPLATE
subroutine update_keys_values_n_states(keys,values,nkeys,dim1,n_st,big_array,lock_2rdm)
use omp_lib
@ -545,7 +545,7 @@ subroutine update_keys_values_n_states(keys,values,nkeys,dim1,n_st,big_array,loc
integer, intent(in) :: keys(4,nkeys)
double precision, intent(in) :: values(n_st,nkeys)
double precision, intent(inout) :: big_array(dim1,dim1,dim1,dim1,n_st)
integer(omp_lock_kind),intent(inout):: lock_2rdm
integer :: istate

228
src/two_rdm_routines/davidson_like_trans_2rdm.irp.f
View File

@ -2,12 +2,12 @@ subroutine orb_range_2_trans_rdm_openmp(big_array,dim1,norb,list_orb,ispin,u_0,N
use bitmasks
implicit none
BEGIN_DOC
! if ispin == 1 :: alpha/alpha 2_rdm
! == 2 :: beta /beta 2_rdm
! == 3 :: alpha/beta + beta/alpha 2trans_rdm
! if ispin == 1 :: alpha/alpha 2_rdm
! == 2 :: beta /beta 2_rdm
! == 3 :: alpha/beta + beta/alpha 2trans_rdm
! == 4 :: spin traced 2_rdm :: aa + bb + ab + ba
!
! notice that here it is the TRANSITION RDM THAT IS COMPUTED
! notice that here it is the TRANSITION RDM THAT IS COMPUTED
!
! THE DIAGONAL PART IS THE USUAL ONE FOR A GIVEN STATE
! Assumes that the determinants are in psi_det
@ -22,7 +22,7 @@ subroutine orb_range_2_trans_rdm_openmp(big_array,dim1,norb,list_orb,ispin,u_0,N
integer :: k
double precision, allocatable :: u_t(:,:)
!DIR$ ATTRIBUTES ALIGN : $IRP_ALIGN :: u_t
PROVIDE mo_two_e_integrals_in_map
PROVIDE all_mo_integrals
allocate(u_t(N_st,N_det))
do k=1,N_st
call dset_order(u_0(1,k),psi_bilinear_matrix_order,N_det)
@ -33,14 +33,14 @@ subroutine orb_range_2_trans_rdm_openmp(big_array,dim1,norb,list_orb,ispin,u_0,N
u_t, &
size(u_t, 1), &
N_det, N_st)
call orb_range_2_trans_rdm_openmp_work(big_array,dim1,norb,list_orb,ispin,u_t,N_st,sze,1,N_det,0,1)
deallocate(u_t)
do k=1,N_st
call dset_order(u_0(1,k),psi_bilinear_matrix_order_reverse,N_det)
enddo
end
subroutine orb_range_2_trans_rdm_openmp_work(big_array,dim1,norb,list_orb,ispin,u_t,N_st,sze,istart,iend,ishift,istep)
@ -55,11 +55,11 @@ subroutine orb_range_2_trans_rdm_openmp_work(big_array,dim1,norb,list_orb,ispin,
integer, intent(in) :: dim1,norb,list_orb(norb),ispin
double precision, intent(inout) :: big_array(dim1,dim1,dim1,dim1,N_st,N_st)
double precision, intent(in) :: u_t(N_st,N_det)
integer :: k
PROVIDE N_int
select case (N_int)
case (1)
call orb_range_2_trans_rdm_openmp_work_1(big_array,dim1,norb,list_orb,ispin,u_t,N_st,sze,istart,iend,ishift,istep)
@ -73,8 +73,8 @@ subroutine orb_range_2_trans_rdm_openmp_work(big_array,dim1,norb,list_orb,ispin,
call orb_range_2_trans_rdm_openmp_work_N_int(big_array,dim1,norb,list_orb,ispin,u_t,N_st,sze,istart,iend,ishift,istep)
end select
end
BEGIN_TEMPLATE
subroutine orb_range_2_trans_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb,ispin,u_t,N_st,sze,istart,iend,ishift,istep)
use bitmasks
@ -82,9 +82,9 @@ subroutine orb_range_2_trans_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb
implicit none
BEGIN_DOC
! Computes the two trans_rdm for the N_st vectors |u_t>
! if ispin == 1 :: alpha/alpha 2trans_rdm
! == 2 :: beta /beta 2trans_rdm
! == 3 :: alpha/beta 2trans_rdm
! if ispin == 1 :: alpha/alpha 2trans_rdm
! == 2 :: beta /beta 2trans_rdm
! == 3 :: alpha/beta 2trans_rdm
! == 4 :: spin traced 2trans_rdm :: aa + bb + 0.5 (ab + ba))
! The 2trans_rdm will be computed only on the list of orbitals list_orb, which contains norb
! Default should be 1,N_det,0,1 for istart,iend,ishift,istep
@ -93,7 +93,7 @@ subroutine orb_range_2_trans_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb
double precision, intent(in) :: u_t(N_st,N_det)
integer, intent(in) :: dim1,norb,list_orb(norb),ispin
double precision, intent(inout) :: big_array(dim1,dim1,dim1,dim1,N_st,N_st)
integer(omp_lock_kind) :: lock_2trans_rdm
integer :: i,j,k,l
integer :: k_a, k_b, l_a, l_b
@ -118,7 +118,7 @@ subroutine orb_range_2_trans_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb
double precision, allocatable :: values(:,:,:)
integer :: nkeys,sze_buff
integer :: ll
alpha_alpha = .False.
alpha_alpha = .False.
beta_beta = .False.
alpha_beta = .False.
spin_trace = .False.
@ -136,27 +136,27 @@ subroutine orb_range_2_trans_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb
stop
endif
PROVIDE N_int
call list_to_bitstring( orb_bitmask, list_orb, norb, N_int)
sze_buff = 6 * norb + elec_alpha_num * elec_alpha_num * 60
list_orb_reverse = -1000
sze_buff = 6 * norb + elec_alpha_num * elec_alpha_num * 60
list_orb_reverse = -1000
do i = 1, norb
list_orb_reverse(list_orb(i)) = i
list_orb_reverse(list_orb(i)) = i
enddo
maxab = max(N_det_alpha_unique, N_det_beta_unique)+1
allocate(idx0(maxab))
do i=1,maxab
idx0(i) = i
enddo
call omp_init_lock(lock_2trans_rdm)
! Prepare the array of all alpha single excitations
! -------------------------------------------------
PROVIDE N_int nthreads_davidson elec_alpha_num
PROVIDE N_int nthreads_davidson elec_alpha_num
!$OMP PARALLEL DEFAULT(NONE) NUM_THREADS(nthreads_davidson) &
!$OMP SHARED(psi_bilinear_matrix_rows, N_det,lock_2trans_rdm,&
!$OMP psi_bilinear_matrix_columns, &
@ -168,7 +168,7 @@ subroutine orb_range_2_trans_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb
!$OMP psi_bilinear_matrix_order_transp_reverse, &
!$OMP psi_bilinear_matrix_columns_loc, &
!$OMP psi_bilinear_matrix_transp_rows_loc,elec_alpha_num, &
!$OMP istart, iend, istep, irp_here,list_orb_reverse, n_states, dim1, &
!$OMP istart, iend, istep, irp_here,list_orb_reverse, n_states, dim1, &
!$OMP ishift, idx0, u_t, maxab, alpha_alpha,beta_beta,alpha_beta,spin_trace,ispin,big_array,sze_buff,orb_bitmask) &
!$OMP PRIVATE(krow, kcol, tmp_det, spindet, k_a, k_b, i,c_1, &
!$OMP lcol, lrow, l_a, l_b, &
@ -176,35 +176,35 @@ subroutine orb_range_2_trans_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb
!$OMP tmp_det2, idx, l, kcol_prev, &
!$OMP singles_a, n_singles_a, singles_b, &
!$OMP n_singles_b, nkeys, keys, values)
! Alpha/Beta double excitations
! =============================
nkeys = 0
allocate( keys(4,sze_buff), values(n_st,n_st,sze_buff))
allocate( keys(4,sze_buff), values(n_st,n_st,sze_buff))
allocate( buffer($N_int,maxab), &
singles_a(maxab), &
singles_b(maxab), &
doubles(maxab), &
idx(maxab))
kcol_prev=-1
ASSERT (iend <= N_det)
ASSERT (istart > 0)
ASSERT (istep > 0)
!$OMP DO SCHEDULE(dynamic,64)
do k_a=istart+ishift,iend,istep
krow = psi_bilinear_matrix_rows(k_a)
ASSERT (krow <= N_det_alpha_unique)
kcol = psi_bilinear_matrix_columns(k_a)
ASSERT (kcol <= N_det_beta_unique)
tmp_det(1:$N_int,1) = psi_det_alpha_unique(1:$N_int, krow)
tmp_det(1:$N_int,2) = psi_det_beta_unique (1:$N_int, kcol)
if (kcol /= kcol_prev) then
call get_all_spin_singles_$N_int( &
psi_det_beta_unique, idx0, &
@ -212,45 +212,45 @@ subroutine orb_range_2_trans_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb
singles_b, n_singles_b)
endif
kcol_prev = kcol
! Loop over singly excited beta columns
! -------------------------------------
do i=1,n_singles_b
lcol = singles_b(i)
tmp_det2(1:$N_int,2) = psi_det_beta_unique(1:$N_int, lcol)
l_a = psi_bilinear_matrix_columns_loc(lcol)
ASSERT (l_a <= N_det)
do j=1,psi_bilinear_matrix_columns_loc(lcol+1) - l_a
lrow = psi_bilinear_matrix_rows(l_a)
ASSERT (lrow <= N_det_alpha_unique)
buffer(1:$N_int,j) = psi_det_alpha_unique(1:$N_int, lrow)
ASSERT (l_a <= N_det)
idx(j) = l_a
l_a = l_a+1
enddo
j = j-1
call get_all_spin_singles_$N_int( &
buffer, idx, tmp_det(1,1), j, &
singles_a, n_singles_a )
! Loop over alpha singles
! -----------------------
if(alpha_beta.or.spin_trace)then
do k = 1,n_singles_a
l_a = singles_a(k)
ASSERT (l_a <= N_det)
lrow = psi_bilinear_matrix_rows(l_a)
ASSERT (lrow <= N_det_alpha_unique)
tmp_det2(1:$N_int,1) = psi_det_alpha_unique(1:$N_int, lrow)
! print*,'nkeys before = ',nkeys
do ll = 1, N_states
@ -259,13 +259,13 @@ subroutine orb_range_2_trans_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb
enddo
enddo
if(alpha_beta)then
! only ONE contribution
! only ONE contribution
if (nkeys+1 .ge. sze_buff) then
call update_keys_values_n_states_trans(keys,values,nkeys,dim1,n_st,big_array,lock_2trans_rdm)
nkeys = 0
endif
else if (spin_trace)then
! TWO contributions
! TWO contributions
if (nkeys+2 .ge. sze_buff) then
call update_keys_values_n_states_trans(keys,values,nkeys,dim1,n_st,big_array,lock_2trans_rdm)
nkeys = 0
@ -275,42 +275,42 @@ subroutine orb_range_2_trans_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb
enddo
endif
call update_keys_values_n_states_trans(keys,values,nkeys,dim1,n_st,big_array,lock_2trans_rdm)
nkeys = 0
enddo
enddo
!$OMP END DO
!$OMP DO SCHEDULE(dynamic,64)
do k_a=istart+ishift,iend,istep
! Single and double alpha exitations
! ===================================
! Initial determinant is at k_a in alpha-major representation
! -----------------------------------------------------------------------
krow = psi_bilinear_matrix_rows(k_a)
ASSERT (krow <= N_det_alpha_unique)
kcol = psi_bilinear_matrix_columns(k_a)
ASSERT (kcol <= N_det_beta_unique)
tmp_det(1:$N_int,1) = psi_det_alpha_unique(1:$N_int, krow)
tmp_det(1:$N_int,2) = psi_det_beta_unique (1:$N_int, kcol)
! Initial determinant is at k_b in beta-major representation
! ----------------------------------------------------------------------
k_b = psi_bilinear_matrix_order_transp_reverse(k_a)
ASSERT (k_b <= N_det)
spindet(1:$N_int) = tmp_det(1:$N_int,1)
! Loop inside the beta column to gather all the connected alphas
lcol = psi_bilinear_matrix_columns(k_a)
l_a = psi_bilinear_matrix_columns_loc(lcol)
@ -320,28 +320,28 @@ subroutine orb_range_2_trans_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb
if (lcol /= kcol) exit
lrow = psi_bilinear_matrix_rows(l_a)
ASSERT (lrow <= N_det_alpha_unique)
buffer(1:$N_int,i) = psi_det_alpha_unique(1:$N_int, lrow)
idx(i) = l_a
l_a = l_a+1
enddo
i = i-1
call get_all_spin_singles_and_doubles_$N_int( &
buffer, idx, spindet, i, &
singles_a, doubles, n_singles_a, n_doubles )
! Compute Hij for all alpha singles
! ----------------------------------
tmp_det2(1:$N_int,2) = psi_det_beta_unique (1:$N_int, kcol)
do i=1,n_singles_a
l_a = singles_a(i)
ASSERT (l_a <= N_det)
lrow = psi_bilinear_matrix_rows(l_a)
ASSERT (lrow <= N_det_alpha_unique)
tmp_det2(1:$N_int,1) = psi_det_alpha_unique(1:$N_int, lrow)
do ll= 1, N_states
do l= 1, N_states
@ -362,23 +362,23 @@ subroutine orb_range_2_trans_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb
endif
call orb_range_off_diag_single_to_all_states_aa_trans_rdm_buffer(tmp_det,tmp_det2,c_1,N_st,orb_bitmask,list_orb_reverse,ispin,sze_buff,nkeys,keys,values)
endif
enddo
call update_keys_values_n_states_trans(keys,values,nkeys,dim1,n_st,big_array,lock_2trans_rdm)
nkeys = 0
! Compute Hij for all alpha doubles
! ----------------------------------
if(alpha_alpha.or.spin_trace)then
do i=1,n_doubles
l_a = doubles(i)
ASSERT (l_a <= N_det)
lrow = psi_bilinear_matrix_rows(l_a)
ASSERT (lrow <= N_det_alpha_unique)
do ll= 1, N_states
do l= 1, N_states
c_1(l,ll) = u_t(ll,l_a) * u_t(l,k_a)
@ -393,29 +393,29 @@ subroutine orb_range_2_trans_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb
endif
call update_keys_values_n_states_trans(keys,values,nkeys,dim1,n_st,big_array,lock_2trans_rdm)
nkeys = 0
! Single and double beta excitations
! ==================================
! Initial determinant is at k_a in alpha-major representation
! -----------------------------------------------------------------------
krow = psi_bilinear_matrix_rows(k_a)
kcol = psi_bilinear_matrix_columns(k_a)
tmp_det(1:$N_int,1) = psi_det_alpha_unique(1:$N_int, krow)
tmp_det(1:$N_int,2) = psi_det_beta_unique (1:$N_int, kcol)
spindet(1:$N_int) = tmp_det(1:$N_int,2)
! Initial determinant is at k_b in beta-major representation
! -----------------------------------------------------------------------
k_b = psi_bilinear_matrix_order_transp_reverse(k_a)
ASSERT (k_b <= N_det)
! Loop inside the alpha row to gather all the connected betas
lrow = psi_bilinear_matrix_transp_rows(k_b)
l_b = psi_bilinear_matrix_transp_rows_loc(lrow)
@ -425,28 +425,28 @@ subroutine orb_range_2_trans_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb
if (lrow /= krow) exit
lcol = psi_bilinear_matrix_transp_columns(l_b)
ASSERT (lcol <= N_det_beta_unique)
buffer(1:$N_int,i) = psi_det_beta_unique(1:$N_int, lcol)
idx(i) = l_b
l_b = l_b+1
enddo
i = i-1
call get_all_spin_singles_and_doubles_$N_int( &
buffer, idx, spindet, i, &
singles_b, doubles, n_singles_b, n_doubles )
! Compute Hij for all beta singles
! ----------------------------------
tmp_det2(1:$N_int,1) = psi_det_alpha_unique(1:$N_int, krow)
do i=1,n_singles_b
l_b = singles_b(i)
ASSERT (l_b <= N_det)
lcol = psi_bilinear_matrix_transp_columns(l_b)
ASSERT (lcol <= N_det_beta_unique)
tmp_det2(1:$N_int,2) = psi_det_beta_unique (1:$N_int, lcol)
l_a = psi_bilinear_matrix_transp_order(l_b)
do ll= 1, N_states
@ -471,18 +471,18 @@ subroutine orb_range_2_trans_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb
enddo
call update_keys_values_n_states_trans(keys,values,nkeys,dim1,n_st,big_array,lock_2trans_rdm)
nkeys = 0
! Compute Hij for all beta doubles
! ----------------------------------
if(beta_beta.or.spin_trace)then
do i=1,n_doubles
l_b = doubles(i)
ASSERT (l_b <= N_det)
lcol = psi_bilinear_matrix_transp_columns(l_b)
ASSERT (lcol <= N_det_beta_unique)
l_a = psi_bilinear_matrix_transp_order(l_b)
do ll= 1, N_states
do l= 1, N_states
@ -496,61 +496,61 @@ subroutine orb_range_2_trans_rdm_openmp_work_$N_int(big_array,dim1,norb,list_orb
call orb_range_off_diag_double_to_all_states_trans_rdm_bb_buffer(tmp_det(1,2),psi_det_beta_unique(1, lcol),c_1,N_st,list_orb_reverse,ispin,sze_buff,nkeys,keys,values)
! print*,'to do orb_range_off_diag_double_to_2_trans_rdm_bb_dm_buffer'
ASSERT (l_a <= N_det)
enddo
endif
call update_keys_values_n_states_trans(keys,values,nkeys,dim1,n_st,big_array,lock_2trans_rdm)
nkeys = 0
! Diagonal contribution
! =====================
! Initial determinant is at k_a in alpha-major representation
! -----------------------------------------------------------------------
krow = psi_bilinear_matrix_rows(k_a)
ASSERT (krow <= N_det_alpha_unique)
kcol = psi_bilinear_matrix_columns(k_a)
ASSERT (kcol <= N_det_beta_unique)
tmp_det(1:$N_int,1) = psi_det_alpha_unique(1:$N_int, krow)
tmp_det(1:$N_int,2) = psi_det_beta_unique (1:$N_int, kcol)
double precision, external :: diag_wee_mat_elem, diag_S_mat_elem
double precision :: c_1(N_states,N_states)
do ll = 1, N_states
do l = 1, N_states
c_1(l,ll) = u_t(ll,k_a) * u_t(l,k_a)
enddo
enddo
call update_keys_values_n_states_trans(keys,values,nkeys,dim1,n_st,big_array,lock_2trans_rdm)
nkeys = 0
call orb_range_diag_to_all_states_2_rdm_trans_buffer(tmp_det,c_1,N_states,orb_bitmask,list_orb_reverse,ispin,sze_buff,nkeys,keys,values)
call update_keys_values_n_states_trans(keys,values,nkeys,dim1,n_st,big_array,lock_2trans_rdm)
nkeys = 0
end do
!$OMP END DO
deallocate(buffer, singles_a, singles_b, doubles, idx, keys, values)
!$OMP END PARALLEL
end
SUBST [ N_int ]
1;;
2;;
3;;
4;;
N_int;;
END_TEMPLATE
subroutine update_keys_values_n_states_trans(keys,values,nkeys,dim1,n_st,big_array,lock_2rdm)
use omp_lib
implicit none
@ -558,7 +558,7 @@ subroutine update_keys_values_n_states_trans(keys,values,nkeys,dim1,n_st,big_arr
integer, intent(in) :: keys(4,nkeys)
double precision, intent(in) :: values(n_st,n_st,nkeys)
double precision, intent(inout) :: big_array(dim1,dim1,dim1,dim1,n_st,n_st)
integer(omp_lock_kind),intent(inout):: lock_2rdm
integer :: i,h1,h2,p1,p2,istate,jstate

26
src/utils_cc/mo_integrals_cc.irp.f
View File

@ -77,7 +77,7 @@ subroutine gen_v_space(n1,n2,n3,n4,list1,list2,list3,list4,v)
else
double precision :: get_two_e_integral
PROVIDE mo_two_e_integrals_in_map
PROVIDE all_mo_integrals
!$OMP PARALLEL &
!$OMP SHARED(n1,n2,n3,n4,list1,list2,list3,list4,v,mo_integrals_map) &
@ -161,7 +161,7 @@ BEGIN_PROVIDER [double precision, cc_space_v, (mo_num,mo_num,mo_num,mo_num)]
integer :: i,j,k,l
double precision :: get_two_e_integral
PROVIDE mo_two_e_integrals_in_map
PROVIDE all_mo_integrals
!$OMP PARALLEL &
!$OMP SHARED(cc_space_v,mo_num,mo_integrals_map) &
@ -194,7 +194,7 @@ BEGIN_PROVIDER [double precision, cc_space_v_oooo, (cc_nOa, cc_nOa, cc_nOa, cc_n
integer :: i1, i2, i3, i4
integer :: n1, n2, n3, n4
n1 = size(cc_space_v_oooo,1)
n2 = size(cc_space_v_oooo,2)
n3 = size(cc_space_v_oooo,3)
@ -237,7 +237,7 @@ BEGIN_PROVIDER [double precision, cc_space_v_vooo, (cc_nVa, cc_nOa, cc_nOa, cc_n
integer :: i1, i2, i3, i4
integer :: n1, n2, n3, n4
n1 = size(cc_space_v_vooo,1)
n2 = size(cc_space_v_vooo,2)
n3 = size(cc_space_v_vooo,3)
@ -281,7 +281,7 @@ BEGIN_PROVIDER [double precision, cc_space_v_ovoo, (cc_nOa, cc_nVa, cc_nOa, cc_n
integer :: i1, i2, i3, i4
integer :: n1, n2, n3, n4
n1 = size(cc_space_v_ovoo,1)
n2 = size(cc_space_v_ovoo,2)
n3 = size(cc_space_v_ovoo,3)
@ -315,7 +315,7 @@ BEGIN_PROVIDER [double precision, cc_space_v_oovo, (cc_nOa, cc_nOa, cc_nVa, cc_n
integer :: i1, i2, i3, i4
integer :: n1, n2, n3, n4
n1 = size(cc_space_v_oovo,1)
n2 = size(cc_space_v_oovo,2)
n3 = size(cc_space_v_oovo,3)
@ -349,7 +349,7 @@ BEGIN_PROVIDER [double precision, cc_space_v_ooov, (cc_nOa, cc_nOa, cc_nOa, cc_n
integer :: i1, i2, i3, i4
integer :: n1, n2, n3, n4
n1 = size(cc_space_v_oovo,1)
n2 = size(cc_space_v_oovo,2)
n3 = size(cc_space_v_oovo,3)
@ -383,7 +383,7 @@ BEGIN_PROVIDER [double precision, cc_space_v_vvoo, (cc_nVa, cc_nVa, cc_nOa, cc_n
integer :: i1, i2, i3, i4
integer :: n1, n2, n3, n4
n1 = size(cc_space_v_vvoo,1)
n2 = size(cc_space_v_vvoo,2)
n3 = size(cc_space_v_vvoo,3)
@ -426,7 +426,7 @@ BEGIN_PROVIDER [double precision, cc_space_v_vovo, (cc_nVa, cc_nOa, cc_nVa, cc_n
integer :: i1, i2, i3, i4
integer :: n1, n2, n3, n4
n1 = size(cc_space_v_vovo,1)
n2 = size(cc_space_v_vovo,2)
n3 = size(cc_space_v_vovo,3)
@ -469,7 +469,7 @@ BEGIN_PROVIDER [double precision, cc_space_v_voov, (cc_nVa, cc_nOa, cc_nOa, cc_n
integer :: i1, i2, i3, i4
integer :: n1, n2, n3, n4
n1 = size(cc_space_v_voov,1)
n2 = size(cc_space_v_voov,2)
n3 = size(cc_space_v_voov,3)
@ -503,7 +503,7 @@ BEGIN_PROVIDER [double precision, cc_space_v_ovvo, (cc_nOa, cc_nVa, cc_nVa, cc_n
integer :: i1, i2, i3, i4
integer :: n1, n2, n3, n4
n1 = size(cc_space_v_ovvo,1)
n2 = size(cc_space_v_ovvo,2)
n3 = size(cc_space_v_ovvo,3)
@ -537,7 +537,7 @@ BEGIN_PROVIDER [double precision, cc_space_v_ovov, (cc_nOa, cc_nVa, cc_nOa, cc_n
integer :: i1, i2, i3, i4
integer :: n1, n2, n3, n4
n1 = size(cc_space_v_ovov,1)
n2 = size(cc_space_v_ovov,2)
n3 = size(cc_space_v_ovov,3)
@ -571,7 +571,7 @@ BEGIN_PROVIDER [double precision, cc_space_v_oovv, (cc_nOa, cc_nOa, cc_nVa, cc_n
integer :: i1, i2, i3, i4
integer :: n1, n2, n3, n4
n1 = size(cc_space_v_oovv,1)
n2 = size(cc_space_v_oovv,2)
n3 = size(cc_space_v_oovv,3)