mirror of
https://github.com/QuantumPackage/qp2.git
synced 2024-12-21 11:03:29 +01:00
commit
51fda32648
@ -14,3 +14,22 @@ type: double precision
|
|||||||
doc: threshold on the weight of a given grid point
|
doc: threshold on the weight of a given grid point
|
||||||
interface: ezfio,provider,ocaml
|
interface: ezfio,provider,ocaml
|
||||||
default: 1.e-20
|
default: 1.e-20
|
||||||
|
|
||||||
|
[my_grid_becke]
|
||||||
|
type: logical
|
||||||
|
doc: if True, the number of angular and radial grid points are read from EZFIO
|
||||||
|
interface: ezfio,provider,ocaml
|
||||||
|
default: False
|
||||||
|
|
||||||
|
[my_n_pt_r_grid]
|
||||||
|
type: integer
|
||||||
|
doc: Number of radial grid points given from input
|
||||||
|
interface: ezfio,provider,ocaml
|
||||||
|
default: 300
|
||||||
|
|
||||||
|
[my_n_pt_a_grid]
|
||||||
|
type: integer
|
||||||
|
doc: Number of angular grid points given from input. Warning, this number cannot be any integer. See file list_angular_grid
|
||||||
|
interface: ezfio,provider,ocaml
|
||||||
|
default: 1202
|
||||||
|
|
||||||
|
@ -8,7 +8,8 @@
|
|||||||
!
|
!
|
||||||
! These numbers are automatically set by setting the grid_type_sgn parameter
|
! These numbers are automatically set by setting the grid_type_sgn parameter
|
||||||
END_DOC
|
END_DOC
|
||||||
select case (grid_type_sgn)
|
if(.not.my_grid_becke)then
|
||||||
|
select case (grid_type_sgn)
|
||||||
case(0)
|
case(0)
|
||||||
n_points_radial_grid = 23
|
n_points_radial_grid = 23
|
||||||
n_points_integration_angular = 170
|
n_points_integration_angular = 170
|
||||||
@ -25,6 +26,10 @@ select case (grid_type_sgn)
|
|||||||
write(*,*) '!!! Quadrature grid not available !!!'
|
write(*,*) '!!! Quadrature grid not available !!!'
|
||||||
stop
|
stop
|
||||||
end select
|
end select
|
||||||
|
else
|
||||||
|
n_points_radial_grid = my_n_pt_r_grid
|
||||||
|
n_points_integration_angular = my_n_pt_a_grid
|
||||||
|
endif
|
||||||
END_PROVIDER
|
END_PROVIDER
|
||||||
|
|
||||||
BEGIN_PROVIDER [integer, n_points_grid_per_atom]
|
BEGIN_PROVIDER [integer, n_points_grid_per_atom]
|
||||||
|
32
src/becke_numerical_grid/list_angular_grid
Normal file
32
src/becke_numerical_grid/list_angular_grid
Normal file
@ -0,0 +1,32 @@
|
|||||||
|
0006
|
||||||
|
0014
|
||||||
|
0026
|
||||||
|
0038
|
||||||
|
0050
|
||||||
|
0074
|
||||||
|
0086
|
||||||
|
0110
|
||||||
|
0146
|
||||||
|
0170
|
||||||
|
0194
|
||||||
|
0230
|
||||||
|
0266
|
||||||
|
0302
|
||||||
|
0350
|
||||||
|
0434
|
||||||
|
0590
|
||||||
|
0770
|
||||||
|
0974
|
||||||
|
1202
|
||||||
|
1454
|
||||||
|
1730
|
||||||
|
2030
|
||||||
|
2354
|
||||||
|
2702
|
||||||
|
3074
|
||||||
|
3470
|
||||||
|
3890
|
||||||
|
4334
|
||||||
|
4802
|
||||||
|
5294
|
||||||
|
5810
|
152
src/cas_based_on_top/two_body_dens_rout.irp.f
Normal file
152
src/cas_based_on_top/two_body_dens_rout.irp.f
Normal file
@ -0,0 +1,152 @@
|
|||||||
|
|
||||||
|
subroutine give_n2_ii_val_ab(r1,r2,two_bod_dens)
|
||||||
|
implicit none
|
||||||
|
BEGIN_DOC
|
||||||
|
! contribution from purely inactive orbitals to n2_{\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):: two_bod_dens
|
||||||
|
integer :: i,j,m,n,i_m,i_n
|
||||||
|
integer :: i_i,i_j
|
||||||
|
double precision, allocatable :: mos_array_inact_r1(:),mos_array_inact_r2(:)
|
||||||
|
double precision, allocatable :: mos_array_r1(:) , mos_array_r2(:)
|
||||||
|
! 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
|
||||||
|
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))
|
||||||
|
enddo
|
||||||
|
do i_m = 1, n_inact_orb
|
||||||
|
mos_array_inact_r2(i_m) = mos_array_r2(list_inact(i_m))
|
||||||
|
enddo
|
||||||
|
|
||||||
|
two_bod_dens = 0.d0
|
||||||
|
! You browse all OCCUPIED ALPHA electrons in the \mathcal{A} space
|
||||||
|
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
|
||||||
|
! 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)
|
||||||
|
enddo
|
||||||
|
enddo
|
||||||
|
end
|
||||||
|
|
||||||
|
|
||||||
|
subroutine give_n2_ia_val_ab(r1,r2,two_bod_dens,istate)
|
||||||
|
BEGIN_DOC
|
||||||
|
! contribution from inactive and active orbitals to n2_{\Psi^B}(r_1,r_2) for the "istate" state of a CAS wave function
|
||||||
|
END_DOC
|
||||||
|
implicit none
|
||||||
|
integer, intent(in) :: istate
|
||||||
|
double precision, intent(in) :: r1(3),r2(3)
|
||||||
|
double precision, intent(out):: 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_inact_r1(:),mos_array_inact_r2(:)
|
||||||
|
double precision, allocatable :: mos_array_act_r1(:),mos_array_act_r2(:)
|
||||||
|
|
||||||
|
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)
|
||||||
|
|
||||||
|
! 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))
|
||||||
|
enddo
|
||||||
|
do i= 1, n_inact_orb
|
||||||
|
mos_array_inact_r2(i) = mos_array_r2(list_inact(i))
|
||||||
|
enddo
|
||||||
|
|
||||||
|
! You extract the active orbitals
|
||||||
|
allocate( mos_array_act_r1(n_act_orb) , mos_array_act_r2(n_act_orb) )
|
||||||
|
do i= 1, n_act_orb
|
||||||
|
mos_array_act_r1(i) = mos_array_r1(list_act(i))
|
||||||
|
enddo
|
||||||
|
do i= 1, n_act_orb
|
||||||
|
mos_array_act_r2(i) = mos_array_r2(list_act(i))
|
||||||
|
enddo
|
||||||
|
|
||||||
|
! Contracted density : intermediate quantity
|
||||||
|
two_bod_dens = 0.d0
|
||||||
|
do a = 1, n_act_orb
|
||||||
|
do i = 1, n_inact_orb
|
||||||
|
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
|
||||||
|
enddo
|
||||||
|
enddo
|
||||||
|
enddo
|
||||||
|
end
|
||||||
|
|
||||||
|
|
||||||
|
subroutine give_n2_aa_val_ab(r1,r2,two_bod_dens,istate)
|
||||||
|
BEGIN_DOC
|
||||||
|
! contribution from purely active orbitals to n2_{\Psi^B}(r_1,r_2) for the "istate" state of a CAS wave function
|
||||||
|
END_DOC
|
||||||
|
implicit none
|
||||||
|
integer, intent(in) :: istate
|
||||||
|
double precision, intent(in) :: r1(3),r2(3)
|
||||||
|
double precision, intent(out):: 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_act_r1(:),mos_array_act_r2(:)
|
||||||
|
|
||||||
|
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)
|
||||||
|
|
||||||
|
! You extract the active orbitals
|
||||||
|
allocate( mos_array_act_r1(n_act_orb) , mos_array_act_r2(n_act_orb) )
|
||||||
|
do i= 1, n_act_orb
|
||||||
|
mos_array_act_r1(i) = mos_array_r1(list_act(i))
|
||||||
|
enddo
|
||||||
|
do i= 1, n_act_orb
|
||||||
|
mos_array_act_r2(i) = mos_array_r2(list_act(i))
|
||||||
|
enddo
|
||||||
|
|
||||||
|
! Contracted density : intermediate quantity
|
||||||
|
two_bod_dens = 0.d0
|
||||||
|
do a = 1, n_act_orb ! 1
|
||||||
|
do b = 1, n_act_orb ! 2
|
||||||
|
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)
|
||||||
|
two_bod_dens += rho * mos_array_act_r1(a) * mos_array_act_r2(b)
|
||||||
|
enddo
|
||||||
|
enddo
|
||||||
|
enddo
|
||||||
|
enddo
|
||||||
|
|
||||||
|
end
|
||||||
|
|
||||||
|
subroutine give_n2_cas(r1,r2,istate,n2_psi)
|
||||||
|
implicit none
|
||||||
|
BEGIN_DOC
|
||||||
|
! returns mu(r), f_psi, n2_psi for a general cas wave function
|
||||||
|
END_DOC
|
||||||
|
integer, intent(in) :: istate
|
||||||
|
double precision, intent(in) :: r1(3),r2(3)
|
||||||
|
double precision, intent(out) :: n2_psi
|
||||||
|
double precision :: two_bod_dens_ii
|
||||||
|
double precision :: two_bod_dens_ia
|
||||||
|
double precision :: two_bod_dens_aa
|
||||||
|
! inactive-inactive part of n2_psi(r1,r2)
|
||||||
|
call give_n2_ii_val_ab(r1,r2,two_bod_dens_ii)
|
||||||
|
! inactive-active part of n2_psi(r1,r2)
|
||||||
|
call give_n2_ia_val_ab(r1,r2,two_bod_dens_ia,istate)
|
||||||
|
! active-active part of n2_psi(r1,r2)
|
||||||
|
call give_n2_aa_val_ab(r1,r2,two_bod_dens_aa,istate)
|
||||||
|
|
||||||
|
n2_psi = two_bod_dens_ii + two_bod_dens_ia + two_bod_dens_aa
|
||||||
|
|
||||||
|
end
|
@ -5,6 +5,7 @@ program casscf
|
|||||||
END_DOC
|
END_DOC
|
||||||
call reorder_orbitals_for_casscf
|
call reorder_orbitals_for_casscf
|
||||||
no_vvvv_integrals = .True.
|
no_vvvv_integrals = .True.
|
||||||
|
touch no_vvvv_integrals
|
||||||
pt2_max = 0.02
|
pt2_max = 0.02
|
||||||
SOFT_TOUCH no_vvvv_integrals pt2_max
|
SOFT_TOUCH no_vvvv_integrals pt2_max
|
||||||
call run_stochastic_cipsi
|
call run_stochastic_cipsi
|
||||||
|
@ -11,3 +11,9 @@ interface: ezfio,provider,ocaml
|
|||||||
default: 1.e-15
|
default: 1.e-15
|
||||||
ezfio_name: threshold_mo
|
ezfio_name: threshold_mo
|
||||||
|
|
||||||
|
[no_vvvv_integrals]
|
||||||
|
type: logical
|
||||||
|
doc: If `True`, computes all integrals except for the integrals having 3 or 4 virtual indices
|
||||||
|
interface: ezfio,provider,ocaml
|
||||||
|
default: false
|
||||||
|
|
||||||
|
@ -1,11 +1,11 @@
|
|||||||
BEGIN_PROVIDER [ logical, no_vvvv_integrals ]
|
!BEGIN_PROVIDER [ logical, no_vvvv_integrals ]
|
||||||
implicit none
|
! implicit none
|
||||||
BEGIN_DOC
|
! BEGIN_DOC
|
||||||
! If `True`, computes all integrals except for the integrals having 3 or 4 virtual indices
|
! If `True`, computes all integrals except for the integrals having 3 or 4 virtual indices
|
||||||
END_DOC
|
! END_DOC
|
||||||
|
!
|
||||||
no_vvvv_integrals = .False.
|
! no_vvvv_integrals = .False.
|
||||||
END_PROVIDER
|
!END_PROVIDER
|
||||||
|
|
||||||
BEGIN_PROVIDER [ double precision, mo_coef_novirt, (ao_num,n_core_inact_act_orb) ]
|
BEGIN_PROVIDER [ double precision, mo_coef_novirt, (ao_num,n_core_inact_act_orb) ]
|
||||||
implicit none
|
implicit none
|
||||||
@ -56,6 +56,8 @@ subroutine four_idx_novvvv
|
|||||||
BEGIN_DOC
|
BEGIN_DOC
|
||||||
! Retransform MO integrals for next CAS-SCF step
|
! Retransform MO integrals for next CAS-SCF step
|
||||||
END_DOC
|
END_DOC
|
||||||
|
print*,'Using partial transformation'
|
||||||
|
print*,'It will not transform all integrals with at least 3 indices within the virtuals'
|
||||||
integer :: i,j,k,l,n_integrals
|
integer :: i,j,k,l,n_integrals
|
||||||
double precision, allocatable :: f(:,:,:), f2(:,:,:), d(:,:), T(:,:,:,:), T2(:,:,:,:)
|
double precision, allocatable :: f(:,:,:), f2(:,:,:), d(:,:), T(:,:,:,:), T2(:,:,:,:)
|
||||||
double precision, external :: get_ao_two_e_integral
|
double precision, external :: get_ao_two_e_integral
|
||||||
|
@ -2,6 +2,8 @@
|
|||||||
BEGIN_PROVIDER [double precision, act_2_rdm_ab_mo, (n_act_orb,n_act_orb,n_act_orb,n_act_orb,N_states)]
|
BEGIN_PROVIDER [double precision, act_2_rdm_ab_mo, (n_act_orb,n_act_orb,n_act_orb,n_act_orb,N_states)]
|
||||||
implicit none
|
implicit none
|
||||||
BEGIN_DOC
|
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 electrons
|
! act_2_rdm_ab_mo(i,j,k,l,istate) = STATE SPECIFIC physicist notation for 2RDM of alpha/beta electrons
|
||||||
!
|
!
|
||||||
! <Psi_{istate}| a^{\dagger}_{i \alpha} a^{\dagger}_{j \beta} a_{l \beta} a_{k \alpha} |Psi_{istate}>
|
! <Psi_{istate}| a^{\dagger}_{i \alpha} a^{\dagger}_{j \beta} a_{l \beta} a_{k \alpha} |Psi_{istate}>
|
||||||
|
@ -75,7 +75,6 @@ subroutine give_explicit_poly_and_gaussian(P_new,P_center,p,fact_k,iorder,alpha,
|
|||||||
P_new(0,1) = 0.d0
|
P_new(0,1) = 0.d0
|
||||||
P_new(0,2) = 0.d0
|
P_new(0,2) = 0.d0
|
||||||
P_new(0,3) = 0.d0
|
P_new(0,3) = 0.d0
|
||||||
|
|
||||||
!DIR$ FORCEINLINE
|
!DIR$ FORCEINLINE
|
||||||
call gaussian_product(alpha,A_center,beta,B_center,fact_k,p,P_center)
|
call gaussian_product(alpha,A_center,beta,B_center,fact_k,p,P_center)
|
||||||
if (fact_k < thresh) then
|
if (fact_k < thresh) then
|
||||||
|
54
src/utils/shank.irp.f
Normal file
54
src/utils/shank.irp.f
Normal file
@ -0,0 +1,54 @@
|
|||||||
|
double precision function shank_general(array,n,nmax)
|
||||||
|
implicit none
|
||||||
|
integer, intent(in) :: n,nmax
|
||||||
|
double precision, intent(in) :: array(0:nmax) ! array of the partial sums
|
||||||
|
integer :: ntmp,i
|
||||||
|
double precision :: sum(0:nmax),shank1(0:nmax)
|
||||||
|
if(n.lt.3)then
|
||||||
|
print*,'You asked to Shank a sum but the order is smaller than 3 ...'
|
||||||
|
print*,'n = ',n
|
||||||
|
print*,'stopping ....'
|
||||||
|
stop
|
||||||
|
endif
|
||||||
|
ntmp = n
|
||||||
|
sum = array
|
||||||
|
i = 0
|
||||||
|
do while(ntmp.ge.2)
|
||||||
|
i += 1
|
||||||
|
! print*,'i = ',i
|
||||||
|
call shank(sum,ntmp,nmax,shank1)
|
||||||
|
ntmp = ntmp - 2
|
||||||
|
sum = shank1
|
||||||
|
shank_general = shank1(ntmp)
|
||||||
|
enddo
|
||||||
|
end
|
||||||
|
|
||||||
|
|
||||||
|
subroutine shank(array,n,nmax,shank1)
|
||||||
|
implicit none
|
||||||
|
integer, intent(in) :: n,nmax
|
||||||
|
double precision, intent(in) :: array(0:nmax)
|
||||||
|
double precision, intent(out) :: shank1(0:nmax)
|
||||||
|
integer :: i,j
|
||||||
|
double precision :: shank_function
|
||||||
|
do i = 1, n-1
|
||||||
|
shank1(i-1) = shank_function(array,i,nmax)
|
||||||
|
enddo
|
||||||
|
end
|
||||||
|
|
||||||
|
double precision function shank_function(array,i,n)
|
||||||
|
implicit none
|
||||||
|
integer, intent(in) :: i,n
|
||||||
|
double precision, intent(in) :: array(0:n)
|
||||||
|
double precision :: b_n, b_n1
|
||||||
|
b_n = array(i) - array(i-1)
|
||||||
|
b_n1 = array(i+1) - array(i)
|
||||||
|
if(dabs(b_n1-b_n).lt.1.d-12)then
|
||||||
|
shank_function = array(i+1)
|
||||||
|
else
|
||||||
|
shank_function = array(i+1) - b_n1*b_n1/(b_n1-b_n)
|
||||||
|
endif
|
||||||
|
|
||||||
|
end
|
||||||
|
|
||||||
|
|
Loading…
Reference in New Issue
Block a user