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Merge branch 'dev' of https://github.com/QuantumPackage/qp2 into dev

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This commit is contained in:
Anthony Scemama 2020-05-15 14:06:38 +02:00
commit f07c2fad45
10 changed files with 281 additions and 9 deletions
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19
src/becke_numerical_grid/EZFIO.cfg
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@ -14,3 +14,22 @@ type: double precision
doc: threshold on the weight of a given grid point
interface: ezfio,provider,ocaml
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

7
src/becke_numerical_grid/grid_becke.irp.f
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@ -8,7 +8,8 @@
!
! These numbers are automatically set by setting the grid_type_sgn parameter
END_DOC
select case (grid_type_sgn)
if(.not.my_grid_becke)then
select case (grid_type_sgn)
case(0)
n_points_radial_grid = 23
n_points_integration_angular = 170
@ -25,6 +26,10 @@ select case (grid_type_sgn)
write(*,*) '!!! Quadrature grid not available !!!'
stop
end select
else
n_points_radial_grid = my_n_pt_r_grid
n_points_integration_angular = my_n_pt_a_grid
endif
END_PROVIDER
BEGIN_PROVIDER [integer, n_points_grid_per_atom]

32
src/becke_numerical_grid/list_angular_grid Normal file
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@ -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
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@ -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

1
src/casscf/casscf.irp.f
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@ -5,6 +5,7 @@ program casscf
END_DOC
call reorder_orbitals_for_casscf
no_vvvv_integrals = .True.
touch no_vvvv_integrals
pt2_max = 0.02
SOFT_TOUCH no_vvvv_integrals pt2_max
call run_stochastic_cipsi

6
src/mo_two_e_ints/EZFIO.cfg
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@ -11,3 +11,9 @@ interface: ezfio,provider,ocaml
default: 1.e-15
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

16
src/mo_two_e_ints/four_idx_novvvv.irp.f
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@ -1,11 +1,11 @@
BEGIN_PROVIDER [ logical, no_vvvv_integrals ]
implicit none
BEGIN_DOC
!BEGIN_PROVIDER [ logical, no_vvvv_integrals ]
! implicit none
! BEGIN_DOC
! If `True`, computes all integrals except for the integrals having 3 or 4 virtual indices
END_DOC
no_vvvv_integrals = .False.
END_PROVIDER
! END_DOC
!
! no_vvvv_integrals = .False.
!END_PROVIDER
BEGIN_PROVIDER [ double precision, mo_coef_novirt, (ao_num,n_core_inact_act_orb) ]
implicit none
@ -56,6 +56,8 @@ subroutine four_idx_novvvv
BEGIN_DOC
! Retransform MO integrals for next CAS-SCF step
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
double precision, allocatable :: f(:,:,:), f2(:,:,:), d(:,:), T(:,:,:,:), T2(:,:,:,:)
double precision, external :: get_ao_two_e_integral

2
src/two_body_rdm/act_2_rdm.irp.f
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@ -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)]
implicit none
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
!
! <Psi_{istate}| a^{\dagger}_{i \alpha} a^{\dagger}_{j \beta} a_{l \beta} a_{k \alpha} |Psi_{istate}>

1
src/utils/integration.irp.f
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@ -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(0,2) = 0.d0
P_new(0,3) = 0.d0
!DIR$ FORCEINLINE
call gaussian_product(alpha,A_center,beta,B_center,fact_k,p,P_center)
if (fact_k < thresh) then

54
src/utils/shank.irp.f Normal file
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@ -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