mirror of
https://github.com/QuantumPackage/qp2.git
synced 2024-08-24 21:21:47 +02:00
added cas_based_on_top
This commit is contained in:
parent
2fc294cd56
commit
87b4eab907
2
src/cas_based_on_top/NEED
Normal file
2
src/cas_based_on_top/NEED
Normal file
@ -0,0 +1,2 @@
|
||||
two_body_rdm
|
||||
dft_utils_in_r
|
9
src/cas_based_on_top/README.rst
Normal file
9
src/cas_based_on_top/README.rst
Normal file
@ -0,0 +1,9 @@
|
||||
==============
|
||||
on_top_density
|
||||
==============
|
||||
|
||||
This plugin proposes different routines/providers to compute the on-top pair density of a CAS-based wave function.
|
||||
|
||||
This means that all determinants in psi_det must belong to an active-space.
|
||||
|
||||
As usual, see the file "example.irp.f" to get introduced to the main providers/routines.
|
125
src/cas_based_on_top/c_i_a_v_mos.irp.f
Normal file
125
src/cas_based_on_top/c_i_a_v_mos.irp.f
Normal file
@ -0,0 +1,125 @@
|
||||
|
||||
BEGIN_PROVIDER[double precision, core_mos_in_r_array, (n_core_orb,n_points_final_grid)]
|
||||
&BEGIN_PROVIDER[double precision, core_mos_in_r_array_transp,(n_points_final_grid,n_core_orb)]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! all COREE MOs on the grid points, arranged in two different ways
|
||||
END_DOC
|
||||
integer :: i,j,k
|
||||
do i = 1, n_core_orb
|
||||
j = list_core(i)
|
||||
do k = 1, n_points_final_grid
|
||||
core_mos_in_r_array_transp(k,i) = mos_in_r_array_transp(k,j)
|
||||
enddo
|
||||
enddo
|
||||
|
||||
do k = 1, n_points_final_grid
|
||||
do i = 1, n_core_orb
|
||||
core_mos_in_r_array(i,k) = core_mos_in_r_array_transp(k,i)
|
||||
enddo
|
||||
enddo
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
|
||||
BEGIN_PROVIDER[double precision, inact_mos_in_r_array, (n_inact_orb,n_points_final_grid)]
|
||||
&BEGIN_PROVIDER[double precision, inact_mos_in_r_array_transp,(n_points_final_grid,n_inact_orb)]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! all INACTIVE MOs on the grid points, arranged in two different ways
|
||||
END_DOC
|
||||
integer :: i,j,k
|
||||
do i = 1, n_inact_orb
|
||||
j = list_inact(i)
|
||||
do k = 1, n_points_final_grid
|
||||
inact_mos_in_r_array_transp(k,i) = mos_in_r_array_transp(k,j)
|
||||
enddo
|
||||
enddo
|
||||
|
||||
do k = 1, n_points_final_grid
|
||||
do i = 1, n_inact_orb
|
||||
inact_mos_in_r_array(i,k) = inact_mos_in_r_array_transp(k,i)
|
||||
enddo
|
||||
enddo
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
BEGIN_PROVIDER[double precision, act_mos_in_r_array, (n_act_orb,n_points_final_grid)]
|
||||
&BEGIN_PROVIDER[double precision, act_mos_in_r_array_transp,(n_points_final_grid,n_act_orb)]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! all ACTIVE MOs on the grid points, arranged in two different ways
|
||||
END_DOC
|
||||
integer :: i,j,k
|
||||
do i = 1, n_act_orb
|
||||
j = list_act(i)
|
||||
do k = 1, n_points_final_grid
|
||||
act_mos_in_r_array_transp(k,i) = mos_in_r_array_transp(k,j)
|
||||
enddo
|
||||
enddo
|
||||
|
||||
do k = 1, n_points_final_grid
|
||||
do i = 1, n_act_orb
|
||||
act_mos_in_r_array(i,k) = act_mos_in_r_array_transp(k,i)
|
||||
enddo
|
||||
enddo
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
|
||||
BEGIN_PROVIDER[double precision, virt_mos_in_r_array, (n_virt_orb,n_points_final_grid)]
|
||||
&BEGIN_PROVIDER[double precision, virt_mos_in_r_array_transp,(n_points_final_grid,n_virt_orb)]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! all VIRTUAL MOs on the grid points, arranged in two different ways
|
||||
END_DOC
|
||||
integer :: i,j,k
|
||||
do i = 1, n_virt_orb
|
||||
j = list_virt(i)
|
||||
do k = 1, n_points_final_grid
|
||||
virt_mos_in_r_array_transp(k,i) = mos_in_r_array_transp(k,j)
|
||||
enddo
|
||||
enddo
|
||||
|
||||
do k = 1, n_points_final_grid
|
||||
do i = 1, n_virt_orb
|
||||
virt_mos_in_r_array(i,k) = virt_mos_in_r_array_transp(k,i)
|
||||
enddo
|
||||
enddo
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
BEGIN_PROVIDER[double precision, core_inact_act_mos_in_r_array, (n_core_inact_act_orb,n_points_final_grid)]
|
||||
&BEGIN_PROVIDER[double precision, core_inact_act_mos_in_r_array_transp,(n_points_final_grid,n_core_inact_act_orb)]
|
||||
implicit none
|
||||
integer :: i,j,k
|
||||
do i = 1, n_core_inact_act_orb
|
||||
j = list_core_inact_act(i)
|
||||
do k = 1, n_points_final_grid
|
||||
core_inact_act_mos_in_r_array_transp(k,i) = mos_in_r_array_transp(k,j)
|
||||
enddo
|
||||
enddo
|
||||
|
||||
do k = 1, n_points_final_grid
|
||||
do i = 1, n_core_inact_act_orb
|
||||
core_inact_act_mos_in_r_array(i,k) = core_inact_act_mos_in_r_array_transp(k,i)
|
||||
enddo
|
||||
enddo
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
BEGIN_PROVIDER[double precision, core_inact_act_mos_grad_in_r_array, (3,n_core_inact_act_orb,n_points_final_grid)]
|
||||
implicit none
|
||||
integer :: i,j,k,l
|
||||
do i = 1, n_core_inact_act_orb
|
||||
j = list_core_inact_act(i)
|
||||
do k = 1, n_points_final_grid
|
||||
do l = 1, 3
|
||||
core_inact_act_mos_grad_in_r_array(l,i,k) = mos_grad_in_r_array(j,k,l)
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
|
47
src/cas_based_on_top/cas_based_density.irp.f
Normal file
47
src/cas_based_on_top/cas_based_density.irp.f
Normal file
@ -0,0 +1,47 @@
|
||||
program cas_based_density
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! TODO : Small example to use the different quantities in this plugin
|
||||
END_DOC
|
||||
|
||||
!! You force QP2 to read the wave function in the EZFIO folder
|
||||
!! It is assumed that all Slater determinants in the wave function
|
||||
!! belongs to an active space defined by core, inactive and active list of orbitals
|
||||
read_wf = .True.
|
||||
touch read_wf
|
||||
call routine_test_cas_based_density
|
||||
|
||||
end
|
||||
|
||||
subroutine routine_test_cas_based_density
|
||||
implicit none
|
||||
integer :: ipoint, istate
|
||||
double precision :: accu_n_elec(N_states),accu_n_elec_2(N_states)
|
||||
|
||||
! PROVIDERS
|
||||
accu_n_elec = 0.d0
|
||||
do istate = 1, N_states
|
||||
do ipoint = 1, n_points_final_grid
|
||||
accu_n_elec(istate) += one_e_cas_total_density(ipoint,istate) * final_weight_at_r_vector(ipoint)
|
||||
enddo
|
||||
print*,'istate = ',istate
|
||||
print*,'accu_n_elec = ',accu_n_elec(istate)
|
||||
enddo
|
||||
|
||||
! ROUTINES
|
||||
double precision :: r(3),core_dens,inact_dens,act_dens(2,N_states),total_cas_dens(N_states)
|
||||
accu_n_elec_2 = 0.d0
|
||||
do ipoint = 1, n_points_final_grid
|
||||
r(:) = final_grid_points(:,ipoint)
|
||||
call give_cas_density_in_r(core_dens,inact_dens,act_dens,total_cas_dens,r)
|
||||
do istate = 1, N_states
|
||||
accu_n_elec_2(istate) += total_cas_dens(istate) * final_weight_at_r_vector(ipoint)
|
||||
enddo
|
||||
enddo
|
||||
|
||||
do istate = 1, N_states
|
||||
print*,'istate = ',istate
|
||||
print*,'accu_n_elec = ',accu_n_elec_2(istate)
|
||||
enddo
|
||||
|
||||
end
|
19
src/cas_based_on_top/cas_based_on_top.irp.f
Normal file
19
src/cas_based_on_top/cas_based_on_top.irp.f
Normal file
@ -0,0 +1,19 @@
|
||||
program cas_based_on_top_density
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! TODO : Small example to use the different quantities in this plugin
|
||||
END_DOC
|
||||
|
||||
!! You force QP2 to read the wave function in the EZFIO folder
|
||||
!! It is assumed that all Slater determinants in the wave function
|
||||
!! belongs to an active space defined by core, inactive and active list of orbitals
|
||||
read_wf = .True.
|
||||
touch read_wf
|
||||
! call routine_test_cas_based_on_top_density
|
||||
call routine
|
||||
end
|
||||
|
||||
subroutine routine
|
||||
implicit none
|
||||
provide total_cas_on_top_density
|
||||
end
|
99
src/cas_based_on_top/cas_dens_prov.irp.f
Normal file
99
src/cas_based_on_top/cas_dens_prov.irp.f
Normal file
@ -0,0 +1,99 @@
|
||||
|
||||
BEGIN_PROVIDER [double precision, one_e_cas_total_density ,(n_points_final_grid,N_states) ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! one_e_cas_total_density = TOTAL DENSITY FOR a CAS wave function
|
||||
!
|
||||
! WARNING : if "no_core_density" == .True. then the core part of density is ignored
|
||||
END_DOC
|
||||
integer :: ipoint,i,j,istate
|
||||
do istate = 1, N_states
|
||||
do ipoint = 1, n_points_final_grid
|
||||
one_e_cas_total_density(ipoint,istate) = one_e_act_density_alpha(ipoint,istate) + one_e_act_density_beta(ipoint,istate) &
|
||||
+ 2.d0 * inact_density(ipoint)
|
||||
if(.not.no_core_density)then !!! YOU ADD THE CORE DENSITY
|
||||
one_e_cas_total_density(ipoint,istate) += 2.d0 * core_density(ipoint)
|
||||
endif
|
||||
enddo
|
||||
enddo
|
||||
END_PROVIDER
|
||||
|
||||
BEGIN_PROVIDER [double precision, one_e_act_density_alpha,(n_points_final_grid,N_states) ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! one_e_act_density_alpha = pure ACTIVE part of the DENSITY for ALPHA ELECTRONS
|
||||
END_DOC
|
||||
one_e_act_density_alpha = 0.d0
|
||||
integer :: ipoint,i,j,istate
|
||||
do istate = 1, N_states
|
||||
do ipoint = 1, n_points_final_grid
|
||||
do i = 1, n_act_orb
|
||||
do j = 1, n_act_orb
|
||||
one_e_act_density_alpha(ipoint,istate) += one_e_act_dm_alpha_mo_for_dft(j,i,istate) * act_mos_in_r_array(j,ipoint) * act_mos_in_r_array(i,ipoint)
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
END_PROVIDER
|
||||
|
||||
|
||||
|
||||
|
||||
BEGIN_PROVIDER [double precision, one_e_act_density_beta,(n_points_final_grid,N_states) ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! one_e_act_density_beta = pure ACTIVE part of the DENSITY for BETA ELECTRONS
|
||||
END_DOC
|
||||
one_e_act_density_beta = 0.d0
|
||||
integer :: ipoint,i,j,istate
|
||||
do istate = 1, N_states
|
||||
do ipoint = 1, n_points_final_grid
|
||||
do i = 1, n_act_orb
|
||||
do j = 1, n_act_orb
|
||||
one_e_act_density_beta(ipoint,istate) += one_e_act_dm_beta_mo_for_dft(j,i,istate) * act_mos_in_r_array(j,ipoint) * act_mos_in_r_array(i,ipoint)
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
END_PROVIDER
|
||||
|
||||
|
||||
|
||||
BEGIN_PROVIDER [double precision, inact_density, (n_points_final_grid) ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! INACTIVE part of the density for alpha/beta.
|
||||
!
|
||||
! WARNING :: IF YOU NEED THE TOTAL DENSITY COMING FROM THE INACTIVE,
|
||||
!
|
||||
! YOU MUST MULTIPLY BY TWO
|
||||
END_DOC
|
||||
integer :: i,j
|
||||
inact_density = 0.d0
|
||||
do i = 1, n_points_final_grid
|
||||
do j = 1, n_inact_orb
|
||||
inact_density(i) += inact_mos_in_r_array(j,i) **2
|
||||
enddo
|
||||
enddo
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
BEGIN_PROVIDER [double precision, core_density, (n_points_final_grid) ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! CORE part of the density for alpha/beta.
|
||||
!
|
||||
! WARNING :: IF YOU NEED THE TOTAL DENSITY COMING FROM THE CORE,
|
||||
!
|
||||
! YOU MUST MULTIPLY BY TWO
|
||||
END_DOC
|
||||
integer :: i,j
|
||||
core_density = 0.d0
|
||||
do i = 1, n_points_final_grid
|
||||
do j = 1, n_core_orb
|
||||
core_density(i) += core_mos_in_r_array(j,i) **2
|
||||
enddo
|
||||
enddo
|
||||
|
||||
END_PROVIDER
|
||||
|
65
src/cas_based_on_top/cas_dens_rout.irp.f
Normal file
65
src/cas_based_on_top/cas_dens_rout.irp.f
Normal file
@ -0,0 +1,65 @@
|
||||
subroutine give_cas_density_in_r(core_dens,inact_dens,act_dens,total_cas_dens,r)
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! returns the different component of the density at grid point r(3) for a CAS wave function
|
||||
!
|
||||
! core_dens : density coming from the CORE orbitals
|
||||
!
|
||||
! inact_dens : density coming from the INACT orbitals
|
||||
!
|
||||
! act_dens(1/2,1:N_states) : active part of the alpha/beta electrons for all states
|
||||
!
|
||||
! total_cas_dens : total density of the cas wave function
|
||||
!
|
||||
! WARNING : if "no_core_density" == .True. then the core part of density is ignored in total_cas_dens
|
||||
END_DOC
|
||||
|
||||
double precision, intent(in) :: r(3)
|
||||
double precision, intent(out) :: core_dens, inact_dens, act_dens(2,N_states), total_cas_dens(N_states)
|
||||
|
||||
double precision, allocatable :: mos_array(:),act_mos(:)
|
||||
allocate(mos_array(mo_num))
|
||||
call give_all_mos_at_r(r,mos_array)
|
||||
integer :: i,iorb,j,jorb,istate
|
||||
|
||||
! core part of the density
|
||||
core_dens = 0.d0
|
||||
do i = 1, n_core_orb
|
||||
iorb = list_core(i)
|
||||
core_dens += mos_array(iorb)*mos_array(iorb)
|
||||
enddo
|
||||
core_dens = core_dens * 2.d0
|
||||
|
||||
! inactive part of the density
|
||||
inact_dens = 0.d0
|
||||
do i = 1, n_inact_orb
|
||||
iorb = list_inact(i)
|
||||
inact_dens += mos_array(iorb)*mos_array(iorb)
|
||||
enddo
|
||||
inact_dens = inact_dens * 2.d0
|
||||
|
||||
allocate(act_mos(n_act_orb))
|
||||
do i = 1, n_act_orb
|
||||
iorb = list_act(i)
|
||||
act_mos(i) = mos_array(iorb)
|
||||
enddo
|
||||
|
||||
! active part of the density for alpha/beta and all states
|
||||
act_dens = 0.d0
|
||||
do istate = 1, N_states
|
||||
do i = 1, n_act_orb
|
||||
do j = 1, n_act_orb
|
||||
act_dens(1,istate) += one_e_act_dm_alpha_mo_for_dft(j,i,istate) * act_mos(j) * act_mos(i)
|
||||
act_dens(2,istate) += one_e_act_dm_beta_mo_for_dft(j,i,istate) * act_mos(j) * act_mos(i)
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
|
||||
! TOTAL density for all states
|
||||
do istate = 1, N_states
|
||||
total_cas_dens(istate) = inact_dens + act_dens(1,istate) + act_dens(2,istate)
|
||||
if(.not.no_core_density)then !!! YOU ADD THE CORE DENSITY
|
||||
total_cas_dens(istate) += core_dens
|
||||
endif
|
||||
enddo
|
||||
end
|
37
src/cas_based_on_top/cas_one_e_rdm.irp.f
Normal file
37
src/cas_based_on_top/cas_one_e_rdm.irp.f
Normal file
@ -0,0 +1,37 @@
|
||||
|
||||
BEGIN_PROVIDER [double precision, one_e_act_dm_beta_mo_for_dft, (n_act_orb,n_act_orb,N_states)]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! one_e_act_dm_beta_mo_for_dft = pure ACTIVE part of the ONE ELECTRON REDUCED DENSITY MATRIX for the BETA ELECTRONS
|
||||
END_DOC
|
||||
integer :: i,j,ii,jj,istate
|
||||
do istate = 1, N_states
|
||||
do ii = 1, n_act_orb
|
||||
i = list_act(ii)
|
||||
do jj = 1, n_act_orb
|
||||
j = list_act(jj)
|
||||
one_e_act_dm_beta_mo_for_dft(jj,ii,istate) = one_e_dm_mo_beta_for_dft(j,i,istate)
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
BEGIN_PROVIDER [double precision, one_e_act_dm_alpha_mo_for_dft, (n_act_orb,n_act_orb,N_states)]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! one_e_act_dm_alpha_mo_for_dft = pure ACTIVE part of the ONE ELECTRON REDUCED DENSITY MATRIX for the ALPHA ELECTRONS
|
||||
END_DOC
|
||||
integer :: i,j,ii,jj,istate
|
||||
do istate = 1, N_states
|
||||
do ii = 1, n_act_orb
|
||||
i = list_act(ii)
|
||||
do jj = 1, n_act_orb
|
||||
j = list_act(jj)
|
||||
one_e_act_dm_alpha_mo_for_dft(jj,ii,istate) = one_e_dm_mo_alpha_for_dft(j,i,istate)
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
|
||||
END_PROVIDER
|
||||
|
68
src/cas_based_on_top/eff_spin_dens.irp.f
Normal file
68
src/cas_based_on_top/eff_spin_dens.irp.f
Normal file
@ -0,0 +1,68 @@
|
||||
BEGIN_PROVIDER [double precision, effective_spin_dm, (n_points_final_grid,N_states) ]
|
||||
&BEGIN_PROVIDER [double precision, grad_effective_spin_dm, (3,n_points_final_grid,N_states) ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! effective_spin_dm(r_i) = \sqrt( n(r)^2 - 4 * ontop(r) )
|
||||
! effective spin density obtained from the total density and on-top pair density
|
||||
! see equation (6) of Phys. Chem. Chem. Phys., 2015, 17, 22412--22422 | 22413
|
||||
END_DOC
|
||||
provide total_cas_on_top_density
|
||||
integer :: i_point,i_state,i
|
||||
double precision :: n2,m2,thr
|
||||
thr = 1.d-14
|
||||
effective_spin_dm = 0.d0
|
||||
grad_effective_spin_dm = 0.d0
|
||||
do i_state = 1, N_states
|
||||
do i_point = 1, n_points_final_grid
|
||||
n2 = (one_e_dm_and_grad_alpha_in_r(4,i_point,i_state) + one_e_dm_and_grad_beta_in_r(4,i_point,i_state))
|
||||
! density squared
|
||||
n2 = n2 * n2
|
||||
if(n2 - 4.D0 * total_cas_on_top_density(i_point,i_state).gt.thr)then
|
||||
effective_spin_dm(i_point,i_state) = dsqrt(n2 - 4.D0 * total_cas_on_top_density(i_point,i_state))
|
||||
if(isnan(effective_spin_dm(i_point,i_state)))then
|
||||
print*,'isnan(effective_spin_dm(i_point,i_state)'
|
||||
stop
|
||||
endif
|
||||
m2 = effective_spin_dm(i_point,i_state)
|
||||
m2 = 0.5d0 / m2 ! 1/(2 * sqrt(n(r)^2 - 4 * ontop(r)) )
|
||||
do i = 1, 3
|
||||
grad_effective_spin_dm(i,i_point,i_state) = m2 * ( one_e_stuff_for_pbe(i,i_point,i_state) - 4.d0 * grad_total_cas_on_top_density(i,i_point,i_state) )
|
||||
enddo
|
||||
else
|
||||
effective_spin_dm(i_point,i_state) = 0.d0
|
||||
grad_effective_spin_dm(:,i_point,i_state) = 0.d0
|
||||
endif
|
||||
enddo
|
||||
enddo
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
|
||||
BEGIN_PROVIDER [double precision, effective_alpha_dm, (n_points_final_grid,N_states) ]
|
||||
&BEGIN_PROVIDER [double precision, effective_beta_dm, (n_points_final_grid,N_states) ]
|
||||
&BEGIN_PROVIDER [double precision, grad_effective_alpha_dm, (3,n_points_final_grid,N_states) ]
|
||||
&BEGIN_PROVIDER [double precision, grad_effective_beta_dm, (3,n_points_final_grid,N_states) ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! effective_alpha_dm(r_i) = 1/2 * (effective_spin_dm(r_i) + n(r_i))
|
||||
! effective_beta_dm(r_i) = 1/2 * (-effective_spin_dm(r_i) + n(r_i))
|
||||
END_DOC
|
||||
provide total_cas_on_top_density
|
||||
integer :: i_point,i_state,i
|
||||
double precision :: n,grad_n
|
||||
do i_state = 1, N_states
|
||||
do i_point = 1, n_points_final_grid
|
||||
n = (one_e_dm_and_grad_alpha_in_r(4,i_point,i_state) + one_e_dm_and_grad_beta_in_r(4,i_point,i_state))
|
||||
effective_alpha_dm(i_point,i_state) = 0.5d0 * (n + effective_spin_dm(i_point,i_state))
|
||||
effective_beta_dm(i_point,i_state) = 0.5d0 * (n - effective_spin_dm(i_point,i_state))
|
||||
do i = 1, 3
|
||||
grad_n = (one_e_dm_and_grad_alpha_in_r(i,i_point,i_state) + one_e_dm_and_grad_beta_in_r(i,i_point,i_state))
|
||||
grad_effective_alpha_dm(i,i_point,i_state) = 0.5d0 * (grad_n + grad_effective_spin_dm(i,i_point,i_state) )
|
||||
grad_effective_beta_dm(i,i_point,i_state) = 0.5d0 * (grad_n - grad_effective_spin_dm(i,i_point,i_state) )
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
|
41
src/cas_based_on_top/example.irp.f
Normal file
41
src/cas_based_on_top/example.irp.f
Normal file
@ -0,0 +1,41 @@
|
||||
|
||||
subroutine write_on_top_in_real_space
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! This routines is a simple example of how to plot the on-top pair density on a simple 1D grid
|
||||
END_DOC
|
||||
double precision :: zmax,dz,r(3),on_top_in_r,total_density,zcenter,dist
|
||||
|
||||
integer :: nz,i,istate
|
||||
character*(128) :: output
|
||||
integer :: i_unit_output,getUnitAndOpen
|
||||
PROVIDE ezfio_filename
|
||||
output=trim(ezfio_filename)//'.on_top'
|
||||
print*,'output = ',trim(output)
|
||||
i_unit_output = getUnitAndOpen(output,'w')
|
||||
|
||||
|
||||
zmax = 2.0d0
|
||||
print*,'nucl_coord(1,3) = ',nucl_coord(1,3)
|
||||
print*,'nucl_coord(2,3) = ',nucl_coord(2,3)
|
||||
dist = dabs(nucl_coord(1,3) - nucl_coord(2,3))
|
||||
zmax += dist
|
||||
zcenter = (nucl_coord(1,3) + nucl_coord(2,3))*0.5d0
|
||||
print*,'zcenter = ',zcenter
|
||||
print*,'zmax = ',zmax
|
||||
nz = 1000
|
||||
dz = zmax / dble(nz)
|
||||
r(:) = 0.d0
|
||||
r(3) = zcenter -zmax * 0.5d0
|
||||
print*,'r(3) = ',r(3)
|
||||
istate = 1
|
||||
do i = 1, nz
|
||||
call give_on_top_in_r_one_state(r,istate,on_top_in_r)
|
||||
call give_cas_density_in_r(r,total_density)
|
||||
write(i_unit_output,*)r(3),on_top_in_r,total_density
|
||||
r(3) += dz
|
||||
enddo
|
||||
|
||||
|
||||
end
|
||||
|
76
src/cas_based_on_top/on_top_cas_prov.irp.f
Normal file
76
src/cas_based_on_top/on_top_cas_prov.irp.f
Normal file
@ -0,0 +1,76 @@
|
||||
|
||||
subroutine act_on_top_on_grid_pt(ipoint,istate,pure_act_on_top_of_r)
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! act_on_top_on_grid_pt returns the purely ACTIVE part of the on top pair density
|
||||
!
|
||||
! at the grid point ipoint, for the state istate
|
||||
END_DOC
|
||||
integer, intent(in) :: ipoint,istate
|
||||
double precision, intent(out) :: pure_act_on_top_of_r
|
||||
double precision :: phi_i,phi_j,phi_k,phi_l
|
||||
integer :: i,j,k,l
|
||||
ASSERT (istate <= N_states)
|
||||
|
||||
pure_act_on_top_of_r = 0.d0
|
||||
do l = 1, n_act_orb
|
||||
phi_l = act_mos_in_r_array(l,ipoint)
|
||||
do k = 1, n_act_orb
|
||||
phi_k = act_mos_in_r_array(k,ipoint)
|
||||
do j = 1, n_act_orb
|
||||
phi_j = act_mos_in_r_array(j,ipoint)
|
||||
do i = 1, n_act_orb
|
||||
phi_i = act_mos_in_r_array(i,ipoint)
|
||||
! 1 2 1 2
|
||||
pure_act_on_top_of_r += act_2_rdm_ab_mo(i,j,k,l,istate) * phi_i * phi_j * phi_k * phi_l
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
end
|
||||
|
||||
|
||||
BEGIN_PROVIDER [double precision, total_cas_on_top_density,(n_points_final_grid,N_states) ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! on top pair density :: n2(r,r) at each of the Becke's grid point of a CAS-BASED wf
|
||||
!
|
||||
! Contains all core/inact/act contribution.
|
||||
!
|
||||
! !!!!! WARNING !!!!! If no_core_density then you REMOVE ALL CONTRIBUTIONS COMING FROM THE CORE ORBITALS
|
||||
END_DOC
|
||||
integer :: i_point,istate
|
||||
double precision :: wall_0,wall_1,core_inact_dm,pure_act_on_top_of_r
|
||||
logical :: no_core
|
||||
print*,'providing the total_cas_on_top_density'
|
||||
! for parallelization
|
||||
provide inact_density core_density one_e_act_density_beta one_e_act_density_alpha act_mos_in_r_array
|
||||
i_point = 1
|
||||
istate = 1
|
||||
call act_on_top_on_grid_pt(i_point,istate,pure_act_on_top_of_r)
|
||||
call wall_time(wall_0)
|
||||
if(no_core_density)then
|
||||
print*,'USING THE VALENCE ONLY TWO BODY DENSITY'
|
||||
endif
|
||||
do istate = 1, N_states
|
||||
!$OMP PARALLEL DO &
|
||||
!$OMP DEFAULT (NONE) &
|
||||
!$OMP PRIVATE (i_point,core_inact_dm,pure_act_on_top_of_r) &
|
||||
!$OMP SHARED(total_cas_on_top_density,n_points_final_grid,inact_density,core_density,one_e_act_density_beta,one_e_act_density_alpha,no_core_density,istate)
|
||||
do i_point = 1, n_points_final_grid
|
||||
call act_on_top_on_grid_pt(i_point,istate,pure_act_on_top_of_r)
|
||||
if(no_core_density) then
|
||||
core_inact_dm = inact_density(i_point)
|
||||
else
|
||||
core_inact_dm = (inact_density(i_point) + core_density(i_point))
|
||||
endif
|
||||
total_cas_on_top_density(i_point,istate) = pure_act_on_top_of_r + core_inact_dm * (one_e_act_density_beta(i_point,istate) + one_e_act_density_alpha(i_point,istate)) + core_inact_dm*core_inact_dm
|
||||
enddo
|
||||
!$OMP END PARALLEL DO
|
||||
enddo
|
||||
call wall_time(wall_1)
|
||||
print*,'provided the total_cas_on_top_density'
|
||||
print*,'Time to provide :',wall_1 - wall_0
|
||||
|
||||
END_PROVIDER
|
||||
|
118
src/cas_based_on_top/on_top_cas_rout.irp.f
Normal file
118
src/cas_based_on_top/on_top_cas_rout.irp.f
Normal file
@ -0,0 +1,118 @@
|
||||
|
||||
subroutine give_core_inact_act_density_in_r(r,mos_array,core_density_in_r,inact_density_in_r,act_density_in_r, total_density)
|
||||
implicit none
|
||||
double precision, intent(in) :: r(3),mos_array(mo_num)
|
||||
double precision, intent(out):: core_density_in_r,inact_density_in_r,act_density_in_r(2,N_states),total_density(N_states)
|
||||
BEGIN_DOC
|
||||
! core, inactive and active part of the density for alpha/beta electrons
|
||||
!
|
||||
! the density coming from the core and inactive are the same for alpha/beta electrons
|
||||
!
|
||||
! act_density(1/2, i) = alpha/beta density for the ith state
|
||||
!
|
||||
! total_density(i) = 2 * (core_density_in_r+inact_density_in_r) + act_density_in_r(1,i) + act_density_in_r(2,i)
|
||||
END_DOC
|
||||
integer :: i,j,istate
|
||||
|
||||
core_density_in_r = 0.d0
|
||||
do i = 1, n_core_orb
|
||||
j = list_core(i)
|
||||
core_density_in_r += mos_array(j) * mos_array(j)
|
||||
enddo
|
||||
|
||||
inact_density_in_r = 0.d0
|
||||
do i = 1, n_inact_orb
|
||||
j = list_inact(i)
|
||||
inact_density_in_r += mos_array(j) * mos_array(j)
|
||||
enddo
|
||||
|
||||
double precision, allocatable :: act_mos(:)
|
||||
double precision :: tmp
|
||||
allocate(act_mos(n_act_orb))
|
||||
do i = 1, n_act_orb
|
||||
j = list_act(i)
|
||||
act_mos(i) = mos_array(j)
|
||||
enddo
|
||||
|
||||
act_density_in_r = 0.d0
|
||||
do istate = 1, N_states
|
||||
do i = 1, n_act_orb
|
||||
do j = 1, n_act_orb
|
||||
tmp = act_mos(i) * act_mos(j)
|
||||
act_density_in_r(1,istate) += tmp * one_e_act_dm_alpha_mo_for_dft(j,i,istate)
|
||||
act_density_in_r(2,istate) += tmp * one_e_act_dm_beta_mo_for_dft(j,i,istate)
|
||||
enddo
|
||||
enddo
|
||||
total_density(istate) = 2.d0 * (core_density_in_r + inact_density_in_r) + act_density_in_r(1,istate) + act_density_in_r(2,istate)
|
||||
enddo
|
||||
|
||||
end
|
||||
|
||||
subroutine give_active_on_top_in_r_one_state(r,istate,mos_array,act_on_top)
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! gives the purely active on-top pair density for a given state
|
||||
END_DOC
|
||||
integer, intent(in) :: istate
|
||||
double precision, intent(in) :: r(3),mos_array(mo_num)
|
||||
double precision, intent(out) :: act_on_top
|
||||
double precision :: phi_i,phi_j,phi_k,phi_l
|
||||
integer :: i,j,k,l
|
||||
|
||||
double precision, allocatable :: act_mos(:)
|
||||
double precision :: tmp
|
||||
allocate(act_mos(n_act_orb))
|
||||
do i = 1, n_act_orb
|
||||
j = list_act(i)
|
||||
act_mos(i) = mos_array(j)
|
||||
enddo
|
||||
|
||||
act_on_top = 0.d0
|
||||
do l = 1, n_act_orb
|
||||
phi_l = act_mos(l)
|
||||
do k = 1, n_act_orb
|
||||
phi_k = act_mos(k)
|
||||
do j = 1, n_act_orb
|
||||
phi_j = act_mos(j)
|
||||
tmp = phi_l * phi_k * phi_j
|
||||
do i = 1, n_act_orb
|
||||
phi_i = act_mos(i)
|
||||
! 1 2 1 2
|
||||
act_on_top += act_2_rdm_ab_mo(i,j,k,l,istate) * tmp * phi_i
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
end
|
||||
|
||||
subroutine give_on_top_in_r_one_state(r,istate,on_top_in_r)
|
||||
implicit none
|
||||
integer, intent(in) :: istate
|
||||
double precision, intent(in) :: r(3)
|
||||
double precision, intent(out) :: on_top_in_r
|
||||
BEGIN_DOC
|
||||
! on top pair density in r for the state istate a CAS-BASED wf
|
||||
!
|
||||
! note that if no_core_density .EQ. .True., all core contributions are excluded
|
||||
END_DOC
|
||||
double precision, allocatable :: mos_array(:)
|
||||
provide act_2_rdm_ab_mo one_e_act_dm_alpha_mo_for_dft one_e_act_dm_beta_mo_for_dft
|
||||
allocate(mos_array(mo_num))
|
||||
call give_all_mos_at_r(r,mos_array)
|
||||
|
||||
double precision :: core_density_in_r, inact_density_in_r, act_density_in_r(2,N_states), total_density(N_states)
|
||||
double precision :: act_on_top,core_inact_dm
|
||||
! getting the different part of the density in r
|
||||
call give_core_inact_act_density_in_r(r,mos_array,core_density_in_r,inact_density_in_r,act_density_in_r, total_density)
|
||||
! getting the purely active part of the density in r
|
||||
call give_active_on_top_in_r_one_state(r,istate,mos_array,act_on_top)
|
||||
|
||||
if(no_core_density) then
|
||||
core_inact_dm = inact_density_in_r
|
||||
else
|
||||
core_inact_dm = core_density_in_r + inact_density_in_r
|
||||
endif
|
||||
on_top_in_r = act_on_top + core_inact_dm * (act_density_in_r(1,istate) + act_density_in_r(2,istate)) + core_inact_dm*core_inact_dm
|
||||
|
||||
end
|
||||
|
73
src/cas_based_on_top/on_top_grad.irp.f
Normal file
73
src/cas_based_on_top/on_top_grad.irp.f
Normal file
@ -0,0 +1,73 @@
|
||||
subroutine give_on_top_gradient(ipoint,istate,ontop_grad)
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! on top pair density and its gradient evaluated at a given point of the grid
|
||||
! ontop_grad(1:3) :: gradients of the on-top pair density
|
||||
! ontop_grad(4) :: on-top pair density
|
||||
END_DOC
|
||||
double precision, intent(out) :: ontop_grad(4)
|
||||
integer, intent(in) :: ipoint,istate
|
||||
double precision :: phi_jkl,phi_ikl,phi_ijl,phi_ijk
|
||||
integer :: i,j,k,l,m
|
||||
|
||||
ontop_grad = 0.d0
|
||||
do l = 1, n_core_inact_act_orb
|
||||
do k = 1, n_core_inact_act_orb
|
||||
do j = 1, n_core_inact_act_orb
|
||||
do i = 1, n_core_inact_act_orb
|
||||
phi_jkl = core_inact_act_mos_in_r_array(j,ipoint) * core_inact_act_mos_in_r_array(k,ipoint) * core_inact_act_mos_in_r_array(l,ipoint)
|
||||
phi_ikl = core_inact_act_mos_in_r_array(i,ipoint) * core_inact_act_mos_in_r_array(k,ipoint) * core_inact_act_mos_in_r_array(l,ipoint)
|
||||
phi_ijl = core_inact_act_mos_in_r_array(i,ipoint) * core_inact_act_mos_in_r_array(j,ipoint) * core_inact_act_mos_in_r_array(l,ipoint)
|
||||
phi_ijk = core_inact_act_mos_in_r_array(i,ipoint) * core_inact_act_mos_in_r_array(j,ipoint) * core_inact_act_mos_in_r_array(k,ipoint)
|
||||
! 1 2 1 2
|
||||
ontop_grad(4) += phi_ijk * core_inact_act_mos_in_r_array(l,ipoint) * full_occ_2_rdm_ab_mo(i,j,k,l,istate)
|
||||
do m = 1,3
|
||||
ontop_grad (m) += full_occ_2_rdm_ab_mo(i,j,k,l,istate) * &
|
||||
( core_inact_act_mos_grad_in_r_array(m,i,ipoint) * phi_jkl + core_inact_act_mos_grad_in_r_array(m,j,ipoint) * phi_ikl + &
|
||||
core_inact_act_mos_grad_in_r_array(m,k,ipoint) * phi_ijl + core_inact_act_mos_grad_in_r_array(m,l,ipoint) * phi_ijk )
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
end
|
||||
|
||||
BEGIN_PROVIDER [double precision, grad_total_cas_on_top_density,(4,n_points_final_grid,N_states) ]
|
||||
&BEGIN_PROVIDER [double precision, wall_time_core_inact_act_on_top_of_r ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! grad_total_cas_on_top_density(1:3,ipoint,istate) : provider for the on top pair density gradient (x,y,z) for the point 'ipoint' and state 'istate'
|
||||
!
|
||||
! grad_total_cas_on_top_density(4,ipoint,istate) : on top pair density for the point 'ipoint' and state 'istate'
|
||||
END_DOC
|
||||
integer :: i_point,i_state,i
|
||||
double precision :: wall_0,wall_1
|
||||
double precision :: core_inact_act_on_top_of_r_from_provider,ontop_grad(4)
|
||||
|
||||
print*,'providing the core_inact_act_on_top_of_r'
|
||||
i_point = 1
|
||||
provide full_occ_2_rdm_ab_mo
|
||||
i_state = 1
|
||||
call give_on_top_gradient(i_point,i_state,ontop_grad)
|
||||
call wall_time(wall_0)
|
||||
!$OMP PARALLEL DO &
|
||||
!$OMP DEFAULT (NONE) &
|
||||
!$OMP PRIVATE (i_point,i_state,ontop_grad) &
|
||||
!$OMP SHARED(grad_total_cas_on_top_density,n_points_final_grid,N_states)
|
||||
do i_point = 1, n_points_final_grid
|
||||
do i_state = 1, N_states
|
||||
call give_on_top_gradient(i_point,i_state,ontop_grad)
|
||||
do i = 1, 4
|
||||
grad_total_cas_on_top_density(i,i_point,i_state) = ontop_grad(i)
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
!$OMP END PARALLEL DO
|
||||
call wall_time(wall_1)
|
||||
print*,'provided the core_inact_act_on_top_of_r'
|
||||
print*,'Time to provide :',wall_1 - wall_0
|
||||
wall_time_core_inact_act_on_top_of_r = wall_1 - wall_0
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
|
Loading…
Reference in New Issue
Block a user