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mirror of https://github.com/LCPQ/quantum_package synced 2024-12-22 20:35:19 +01:00

updated NEEDED_MODULES in src repository

This commit is contained in:
Manu 2015-03-18 11:35:16 +01:00
parent a4593d7e17
commit 6a6c197b9a
6 changed files with 159 additions and 4 deletions

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@ -23,6 +23,7 @@ deinit_thread
skip
init_main
filter_integrals
filter2h2p
""".split()
class H_apply(object):
@ -115,6 +116,13 @@ class H_apply(object):
buffer = buffer.replace('$'+key, value)
return buffer
def set_filter_2h_2p(self):
self["filter2h2p"] = """
! ! DIR$ FORCEINLINE
if(is_a_two_holes_two_particles(key))cycle
"""
def set_perturbation(self,pert):
if self.perturbation is not None:
raise

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@ -276,6 +276,7 @@ double precision function get_mo_bielec_integral(i,j,k,l,map)
implicit none
BEGIN_DOC
! Returns one integral <ij|kl> in the MO basis
! i(1)j(1) 1/r12 k(2)l(2)
END_DOC
integer, intent(in) :: i,j,k,l
integer*8 :: idx
@ -292,6 +293,7 @@ double precision function mo_bielec_integral(i,j,k,l)
implicit none
BEGIN_DOC
! Returns one integral <ij|kl> in the MO basis
! i(1)j(1) 1/r12 k(2)l(2)
END_DOC
integer, intent(in) :: i,j,k,l
double precision :: get_mo_bielec_integral
@ -306,6 +308,7 @@ subroutine get_mo_bielec_integrals(j,k,l,sze,out_val,map)
BEGIN_DOC
! Returns multiple integrals <ij|kl> in the MO basis, all
! i for j,k,l fixed.
! i(1)j(1) 1/r12 k(2)l(2)
END_DOC
integer, intent(in) :: j,k,l, sze
real(integral_kind), intent(out) :: out_val(sze)
@ -327,6 +330,7 @@ subroutine get_mo_bielec_integrals_existing_ik(j,l,sze,out_array,map)
implicit none
BEGIN_DOC
! Returns multiple integrals <ij|kl> in the MO basis, all
! i(1)j(1) 1/r12 k(2)l(2)
! i for j,k,l fixed.
END_DOC
integer, intent(in) :: j,l, sze

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@ -26,6 +26,7 @@ subroutine $subroutine_diexc(key_in, hole_1,particl_1, hole_2, particl_2, i_gene
integer :: N_elec_in_key_hole_2(2),N_elec_in_key_part_2(2)
double precision :: mo_bielec_integral
logical :: is_a_two_holes_two_particles
integer, allocatable :: ia_ja_pairs(:,:,:)
integer, allocatable :: ib_jb_pairs(:,:)
double precision :: diag_H_mat_elem
@ -162,6 +163,7 @@ subroutine $subroutine_diexc(key_in, hole_1,particl_1, hole_2, particl_2, i_gene
k = ishft(j_b-1,-bit_kind_shift)+1
l = j_b-ishft(k-1,bit_kind_shift)-1
key(k,other_spin) = ibset(key(k,other_spin),l)
$filter2h2p
key_idx += 1
do k=1,N_int
keys_out(k,1,key_idx) = key(k,1)
@ -210,6 +212,7 @@ subroutine $subroutine_diexc(key_in, hole_1,particl_1, hole_2, particl_2, i_gene
k = ishft(j_b-1,-bit_kind_shift)+1
l = j_b-ishft(k-1,bit_kind_shift)-1
key(k,ispin) = ibset(key(k,ispin),l)
$filter2h2p
key_idx += 1
do k=1,N_int
keys_out(k,1,key_idx) = key(k,1)
@ -267,6 +270,7 @@ subroutine $subroutine_monoexc(key_in, hole_1,particl_1,i_generator,iproc $param
integer :: kk,pp,other_spin,key_idx
integer :: N_elec_in_key_hole_1(2),N_elec_in_key_part_1(2)
integer :: N_elec_in_key_hole_2(2),N_elec_in_key_part_2(2)
logical :: is_a_two_holes_two_particles
integer, allocatable :: ia_ja_pairs(:,:,:)
logical, allocatable :: array_pairs(:,:)
@ -333,6 +337,7 @@ subroutine $subroutine_monoexc(key_in, hole_1,particl_1,i_generator,iproc $param
k_a = ishft(j_a-1,-bit_kind_shift)+1
l_a = j_a-ishft(k_a-1,bit_kind_shift)-1
hole(k_a,ispin) = ibset(hole(k_a,ispin),l_a)
$filter2h2p
key_idx += 1
do k=1,N_int
keys_out(k,1,key_idx) = hole(k,1)

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@ -0,0 +1,138 @@
program pouet
implicit none
print*,'HF energy = ',ref_bitmask_energy + nuclear_repulsion
call routine
end
subroutine routine
use bitmasks
implicit none
integer :: i,j,k,l
double precision :: hij,get_mo_bielec_integral
double precision :: hmono,h_bi_ispin,h_bi_other_spin
integer(bit_kind),allocatable :: key_tmp(:,:)
integer, allocatable :: occ(:,:)
integer :: n_occ_alpha, n_occ_beta
! First checks
print*,'N_int = ',N_int
print*,'mo_tot_num = ',mo_tot_num
print*,'mo_tot_num / 64+1= ',mo_tot_num/64+1
! We print the HF determinant
do i = 1, N_int
print*,'ref_bitmask(i,1) = ',ref_bitmask(i,1)
print*,'ref_bitmask(i,2) = ',ref_bitmask(i,2)
enddo
print*,''
print*,'Hartree Fock determinant ...'
call debug_det(ref_bitmask,N_int)
allocate(key_tmp(N_int,2))
! We initialize key_tmp to the Hartree Fock one
key_tmp = ref_bitmask
integer :: i_hole,i_particle,ispin,i_ok,other_spin
! We do a mono excitation on the top of the HF determinant
write(*,*)'Enter the (hole, particle) couple for the mono excitation ...'
read(5,*)i_hole,i_particle
!!i_hole = 4
!!i_particle = 20
write(*,*)'Enter the ispin variable ...'
write(*,*)'ispin = 1 ==> alpha '
write(*,*)'ispin = 2 ==> beta '
read(5,*)ispin
if(ispin == 1)then
other_spin = 2
else if(ispin == 2)then
other_spin = 1
else
print*,'PB !! '
print*,'ispin must be 1 or 2 !'
stop
endif
!!ispin = 1
call do_mono_excitation(key_tmp,i_hole,i_particle,ispin,i_ok)
! We check if it the excitation was possible with "i_ok"
if(i_ok == -1)then
print*,'i_ok = ',i_ok
print*,'You can not do this excitation because of Pauli principle ...'
print*,'check your hole particle couple, there must be something wrong ...'
stop
endif
print*,'New det = '
call debug_det(key_tmp,N_int)
call i_H_j(key_tmp,ref_bitmask,N_int,hij)
! We calculate the H matrix element between the new determinant and HF
print*,'<D_i|H|D_j> = ',hij
print*,''
print*,''
print*,'Recalculating it old school style ....'
print*,''
print*,''
! We recalculate this old school style !!!
! Mono electronic part
hmono = mo_mono_elec_integral(i_hole,i_particle)
print*,''
print*,'Mono electronic part '
print*,''
print*,'<D_i|h(1)|D_j> = ',hmono
h_bi_ispin = 0.d0
h_bi_other_spin = 0.d0
print*,''
print*,'Getting all the info for the calculation of the bi electronic part ...'
print*,''
allocate (occ(N_int*bit_kind_size,2))
! We get the occupation of the alpha electrons in occ(:,1)
call bitstring_to_list(key_tmp(1,1), occ(1,1), n_occ_alpha, N_int)
print*,'n_occ_alpha = ',n_occ_alpha
print*,'elec_alpha_num = ',elec_alpha_num
! We get the occupation of the beta electrons in occ(:,2)
call bitstring_to_list(key_tmp(1,2), occ(1,2), n_occ_beta, N_int)
print*,'n_occ_beta = ',n_occ_beta
print*,'elec_beta_num = ',elec_beta_num
! We print the occupation of the alpha electrons
print*,'Alpha electrons !'
do i = 1, n_occ_alpha
print*,'i = ',i
print*,'occ(i,1) = ',occ(i,1)
enddo
! We print the occupation of the beta electrons
print*,'Alpha electrons !'
do i = 1, n_occ_beta
print*,'i = ',i
print*,'occ(i,2) = ',occ(i,2)
enddo
integer :: exc(0:2,2,2),degree,h1,p1,h2,p2,s1,s2
double precision :: phase
call get_excitation_degree(key_tmp,ref_bitmask,degree,N_int)
print*,'degree = ',degree
call get_mono_excitation(ref_bitmask,key_tmp,exc,phase,N_int)
call decode_exc(exc,degree,h1,p1,h2,p2,s1,s2)
print*,'h1 = ',h1
print*,'p1 = ',p1
print*,'s1 = ',s1
print*,'phase = ',phase
do i = 1, elec_num_tab(ispin)
integer :: orb_occupied
orb_occupied = occ(i,ispin)
h_bi_ispin += get_mo_bielec_integral(i_hole,orb_occupied,i_particle,orb_occupied,mo_integrals_map) &
-get_mo_bielec_integral(i_hole,i_particle,orb_occupied,orb_occupied,mo_integrals_map)
enddo
print*,'h_bi_ispin = ',h_bi_ispin
do i = 1, elec_num_tab(other_spin)
orb_occupied = occ(i,other_spin)
h_bi_other_spin += get_mo_bielec_integral(i_hole,orb_occupied,i_particle,orb_occupied,mo_integrals_map)
enddo
print*,'h_bi_other_spin = ',h_bi_other_spin
print*,'h_bi_ispin + h_bi_other_spin = ',h_bi_ispin + h_bi_other_spin
print*,'Total matrix element = ',phase*(h_bi_ispin + h_bi_other_spin + hmono)
!i = 1
!j = 1
!k = 1
!l = 1
!hij = get_mo_bielec_integral(i,j,k,l,mo_integrals_map)
!print*,'<ij|kl> = ',hij
end

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@ -11,11 +11,11 @@ BEGIN_PROVIDER [double precision, mo_nucl_elec_integral, (mo_tot_num_align,mo_to
do i = 1, mo_tot_num
do j = 1, mo_tot_num
do i1 = 1,ao_num
c_i1 = mo_coef(i1,i)
c_i1 = mo_coef(i1,i) ! <AO(i1)|MO(i)>
do j1 = 1,ao_num
c_j1 = c_i1*mo_coef(j1,j)
c_j1 = c_i1*mo_coef(j1,j) ! <AO(j1)|MO(j)>
mo_nucl_elec_integral(j,i) = mo_nucl_elec_integral(j,i) + &
c_j1 * ao_nucl_elec_integral(j1,i1)
c_j1 * ao_nucl_elec_integral(j1,i1)
enddo
enddo
enddo

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@ -1 +1 @@
AOs BiInts Bitmask Dets Electrons Ezfio_files Full_CI Generators_full Hartree_Fock MOGuess MonoInts MOs Nuclei Output Selectors_full Utils Molden FCIdump Generators_CAS
AOs BiInts Bitmask Dets Electrons Ezfio_files Full_CI Generators_full Hartree_Fock MOGuess MonoInts MOs Nuclei Output Selectors_full Utils Molden FCIdump Generators_CAS Denstity_stuff CAS_SD_selected DDCI_selected Two_body_density_matrix