mirror of
https://github.com/QuantumPackage/qp2.git
synced 2024-11-07 05:53:37 +01:00
commit
51fda32648
@ -14,3 +14,22 @@ type: double precision
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doc: threshold on the weight of a given grid point
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doc: threshold on the weight of a given grid point
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interface: ezfio,provider,ocaml
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interface: ezfio,provider,ocaml
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default: 1.e-20
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default: 1.e-20
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[my_grid_becke]
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type: logical
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doc: if True, the number of angular and radial grid points are read from EZFIO
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interface: ezfio,provider,ocaml
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default: False
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[my_n_pt_r_grid]
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type: integer
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doc: Number of radial grid points given from input
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interface: ezfio,provider,ocaml
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default: 300
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[my_n_pt_a_grid]
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type: integer
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doc: Number of angular grid points given from input. Warning, this number cannot be any integer. See file list_angular_grid
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interface: ezfio,provider,ocaml
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default: 1202
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@ -8,6 +8,7 @@
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!
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!
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! These numbers are automatically set by setting the grid_type_sgn parameter
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! These numbers are automatically set by setting the grid_type_sgn parameter
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END_DOC
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END_DOC
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if(.not.my_grid_becke)then
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select case (grid_type_sgn)
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select case (grid_type_sgn)
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case(0)
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case(0)
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n_points_radial_grid = 23
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n_points_radial_grid = 23
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@ -25,6 +26,10 @@ select case (grid_type_sgn)
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write(*,*) '!!! Quadrature grid not available !!!'
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write(*,*) '!!! Quadrature grid not available !!!'
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stop
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stop
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end select
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end select
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else
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n_points_radial_grid = my_n_pt_r_grid
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n_points_integration_angular = my_n_pt_a_grid
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endif
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END_PROVIDER
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END_PROVIDER
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BEGIN_PROVIDER [integer, n_points_grid_per_atom]
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BEGIN_PROVIDER [integer, n_points_grid_per_atom]
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32
src/becke_numerical_grid/list_angular_grid
Normal file
32
src/becke_numerical_grid/list_angular_grid
Normal file
@ -0,0 +1,32 @@
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0006
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0014
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0026
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0038
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0050
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0074
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0086
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0110
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0146
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0170
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0194
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0230
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0266
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0302
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0350
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0434
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0590
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0770
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0974
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1202
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1454
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1730
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2030
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2354
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2702
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3074
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3470
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3890
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4334
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4802
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5294
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5810
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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 @@
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subroutine give_n2_ii_val_ab(r1,r2,two_bod_dens)
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implicit none
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BEGIN_DOC
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! contribution from purely inactive orbitals to n2_{\Psi^B}(r_1,r_2) for a CAS wave function
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END_DOC
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double precision, intent(in) :: r1(3),r2(3)
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double precision, intent(out):: two_bod_dens
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integer :: i,j,m,n,i_m,i_n
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integer :: i_i,i_j
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double precision, allocatable :: mos_array_inact_r1(:),mos_array_inact_r2(:)
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double precision, allocatable :: mos_array_r1(:) , mos_array_r2(:)
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! You get all orbitals in r_1 and r_2
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allocate(mos_array_r1(mo_num) , mos_array_r2(mo_num) )
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call give_all_mos_at_r(r1,mos_array_r1)
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call give_all_mos_at_r(r2,mos_array_r2)
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! You extract the inactive orbitals
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allocate(mos_array_inact_r1(n_inact_orb) , mos_array_inact_r2(n_inact_orb) )
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do i_m = 1, n_inact_orb
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mos_array_inact_r1(i_m) = mos_array_r1(list_inact(i_m))
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enddo
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do i_m = 1, n_inact_orb
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mos_array_inact_r2(i_m) = mos_array_r2(list_inact(i_m))
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enddo
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two_bod_dens = 0.d0
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! You browse all OCCUPIED ALPHA electrons in the \mathcal{A} space
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do m = 1, n_inact_orb ! electron 1
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! You browse all OCCUPIED BETA electrons in the \mathcal{A} space
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do n = 1, n_inact_orb ! electron 2
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! two_bod_dens(r_1,r_2) = n_alpha(r_1) * n_beta(r_2)
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two_bod_dens += mos_array_inact_r1(m) * mos_array_inact_r1(m) * mos_array_inact_r2(n) * mos_array_inact_r2(n)
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enddo
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enddo
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end
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subroutine give_n2_ia_val_ab(r1,r2,two_bod_dens,istate)
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BEGIN_DOC
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! contribution from inactive and active orbitals to n2_{\Psi^B}(r_1,r_2) for the "istate" state of a CAS wave function
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END_DOC
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implicit none
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integer, intent(in) :: istate
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double precision, intent(in) :: r1(3),r2(3)
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double precision, intent(out):: two_bod_dens
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integer :: i,orb_i,a,orb_a,n,m,b
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double precision :: rho
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double precision, allocatable :: mos_array_r1(:) , mos_array_r2(:)
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double precision, allocatable :: mos_array_inact_r1(:),mos_array_inact_r2(:)
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double precision, allocatable :: mos_array_act_r1(:),mos_array_act_r2(:)
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two_bod_dens = 0.d0
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! You get all orbitals in r_1 and r_2
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allocate(mos_array_r1(mo_num) , mos_array_r2(mo_num) )
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call give_all_mos_at_r(r1,mos_array_r1)
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call give_all_mos_at_r(r2,mos_array_r2)
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! You extract the inactive orbitals
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allocate( mos_array_inact_r1(n_inact_orb) , mos_array_inact_r2(n_inact_orb) )
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do i = 1, n_inact_orb
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mos_array_inact_r1(i) = mos_array_r1(list_inact(i))
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enddo
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do i= 1, n_inact_orb
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mos_array_inact_r2(i) = mos_array_r2(list_inact(i))
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enddo
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! You extract the active orbitals
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allocate( mos_array_act_r1(n_act_orb) , mos_array_act_r2(n_act_orb) )
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do i= 1, n_act_orb
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mos_array_act_r1(i) = mos_array_r1(list_act(i))
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enddo
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do i= 1, n_act_orb
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mos_array_act_r2(i) = mos_array_r2(list_act(i))
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enddo
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! Contracted density : intermediate quantity
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two_bod_dens = 0.d0
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do a = 1, n_act_orb
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do i = 1, n_inact_orb
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do b = 1, n_act_orb
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rho = one_e_act_dm_beta_mo_for_dft(b,a,istate) + one_e_act_dm_alpha_mo_for_dft(b,a,istate)
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two_bod_dens += mos_array_inact_r1(i) * mos_array_inact_r1(i) * mos_array_act_r2(a) * mos_array_act_r2(b) * rho
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enddo
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enddo
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enddo
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end
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subroutine give_n2_aa_val_ab(r1,r2,two_bod_dens,istate)
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BEGIN_DOC
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! contribution from purely active orbitals to n2_{\Psi^B}(r_1,r_2) for the "istate" state of a CAS wave function
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END_DOC
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implicit none
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integer, intent(in) :: istate
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double precision, intent(in) :: r1(3),r2(3)
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double precision, intent(out):: two_bod_dens
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integer :: i,orb_i,a,orb_a,n,m,b,c,d
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double precision :: rho
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double precision, allocatable :: mos_array_r1(:) , mos_array_r2(:)
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double precision, allocatable :: mos_array_act_r1(:),mos_array_act_r2(:)
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two_bod_dens = 0.d0
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! You get all orbitals in r_1 and r_2
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allocate(mos_array_r1(mo_num) , mos_array_r2(mo_num) )
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call give_all_mos_at_r(r1,mos_array_r1)
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call give_all_mos_at_r(r2,mos_array_r2)
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! You extract the active orbitals
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allocate( mos_array_act_r1(n_act_orb) , mos_array_act_r2(n_act_orb) )
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do i= 1, n_act_orb
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mos_array_act_r1(i) = mos_array_r1(list_act(i))
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enddo
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do i= 1, n_act_orb
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mos_array_act_r2(i) = mos_array_r2(list_act(i))
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enddo
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! Contracted density : intermediate quantity
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two_bod_dens = 0.d0
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do a = 1, n_act_orb ! 1
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do b = 1, n_act_orb ! 2
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do c = 1, n_act_orb ! 1
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do d = 1, n_act_orb ! 2
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rho = mos_array_act_r1(c) * mos_array_act_r2(d) * act_2_rdm_ab_mo(d,c,b,a,istate)
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two_bod_dens += rho * mos_array_act_r1(a) * mos_array_act_r2(b)
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enddo
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enddo
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enddo
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enddo
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end
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subroutine give_n2_cas(r1,r2,istate,n2_psi)
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implicit none
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BEGIN_DOC
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! returns mu(r), f_psi, n2_psi for a general cas wave function
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END_DOC
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integer, intent(in) :: istate
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double precision, intent(in) :: r1(3),r2(3)
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double precision, intent(out) :: n2_psi
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double precision :: two_bod_dens_ii
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double precision :: two_bod_dens_ia
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double precision :: two_bod_dens_aa
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! inactive-inactive part of n2_psi(r1,r2)
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call give_n2_ii_val_ab(r1,r2,two_bod_dens_ii)
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! inactive-active part of n2_psi(r1,r2)
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call give_n2_ia_val_ab(r1,r2,two_bod_dens_ia,istate)
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! active-active part of n2_psi(r1,r2)
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call give_n2_aa_val_ab(r1,r2,two_bod_dens_aa,istate)
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n2_psi = two_bod_dens_ii + two_bod_dens_ia + two_bod_dens_aa
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end
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@ -5,6 +5,7 @@ program casscf
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END_DOC
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END_DOC
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call reorder_orbitals_for_casscf
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call reorder_orbitals_for_casscf
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no_vvvv_integrals = .True.
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no_vvvv_integrals = .True.
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touch no_vvvv_integrals
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pt2_max = 0.02
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pt2_max = 0.02
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SOFT_TOUCH no_vvvv_integrals pt2_max
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SOFT_TOUCH no_vvvv_integrals pt2_max
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call run_stochastic_cipsi
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call run_stochastic_cipsi
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@ -11,3 +11,9 @@ interface: ezfio,provider,ocaml
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default: 1.e-15
|
default: 1.e-15
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ezfio_name: threshold_mo
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ezfio_name: threshold_mo
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[no_vvvv_integrals]
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type: logical
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doc: If `True`, computes all integrals except for the integrals having 3 or 4 virtual indices
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interface: ezfio,provider,ocaml
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default: false
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@ -1,11 +1,11 @@
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BEGIN_PROVIDER [ logical, no_vvvv_integrals ]
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!BEGIN_PROVIDER [ logical, no_vvvv_integrals ]
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implicit none
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! implicit none
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BEGIN_DOC
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! BEGIN_DOC
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! If `True`, computes all integrals except for the integrals having 3 or 4 virtual indices
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! If `True`, computes all integrals except for the integrals having 3 or 4 virtual indices
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END_DOC
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! END_DOC
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!
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no_vvvv_integrals = .False.
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! no_vvvv_integrals = .False.
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END_PROVIDER
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!END_PROVIDER
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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) ]
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implicit none
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implicit none
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@ -56,6 +56,8 @@ subroutine four_idx_novvvv
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BEGIN_DOC
|
BEGIN_DOC
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! Retransform MO integrals for next CAS-SCF step
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! Retransform MO integrals for next CAS-SCF step
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END_DOC
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END_DOC
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print*,'Using partial transformation'
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print*,'It will not transform all integrals with at least 3 indices within the virtuals'
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integer :: i,j,k,l,n_integrals
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integer :: i,j,k,l,n_integrals
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double precision, allocatable :: f(:,:,:), f2(:,:,:), d(:,:), T(:,:,:,:), T2(:,:,:,:)
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double precision, allocatable :: f(:,:,:), f2(:,:,:), d(:,:), T(:,:,:,:), T2(:,:,:,:)
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double precision, external :: get_ao_two_e_integral
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double precision, external :: get_ao_two_e_integral
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|
@ -2,6 +2,8 @@
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BEGIN_PROVIDER [double precision, act_2_rdm_ab_mo, (n_act_orb,n_act_orb,n_act_orb,n_act_orb,N_states)]
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BEGIN_PROVIDER [double precision, act_2_rdm_ab_mo, (n_act_orb,n_act_orb,n_act_orb,n_act_orb,N_states)]
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implicit none
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implicit none
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BEGIN_DOC
|
BEGIN_DOC
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||||||
|
! 12 12
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|
! 1 2 1 2 == <ij|kl>
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! 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
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!
|
!
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! <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}>
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|
@ -75,7 +75,6 @@ subroutine give_explicit_poly_and_gaussian(P_new,P_center,p,fact_k,iorder,alpha,
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P_new(0,1) = 0.d0
|
P_new(0,1) = 0.d0
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P_new(0,2) = 0.d0
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P_new(0,2) = 0.d0
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P_new(0,3) = 0.d0
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P_new(0,3) = 0.d0
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|
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!DIR$ FORCEINLINE
|
!DIR$ FORCEINLINE
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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)
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if (fact_k < thresh) then
|
if (fact_k < thresh) then
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|
54
src/utils/shank.irp.f
Normal file
54
src/utils/shank.irp.f
Normal file
@ -0,0 +1,54 @@
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|
double precision function shank_general(array,n,nmax)
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|
implicit none
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|
integer, intent(in) :: n,nmax
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|
double precision, intent(in) :: array(0:nmax) ! array of the partial sums
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|
integer :: ntmp,i
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|
double precision :: sum(0:nmax),shank1(0:nmax)
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|
if(n.lt.3)then
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|
print*,'You asked to Shank a sum but the order is smaller than 3 ...'
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|
print*,'n = ',n
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||||||
|
print*,'stopping ....'
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|
stop
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|
endif
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|
ntmp = n
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|
sum = array
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|
i = 0
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do while(ntmp.ge.2)
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|
i += 1
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|
! print*,'i = ',i
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|
call shank(sum,ntmp,nmax,shank1)
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||||||
|
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