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https://github.com/QuantumPackage/qp2.git
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Merge branch 'dev' of github.com:QuantumPackage/qp2 into dev
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commit
fa4cb043ee
1
etc/openmp.rc
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1
etc/openmp.rc
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export OMP_NESTED=True
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2
external/qp2-dependencies
vendored
2
external/qp2-dependencies
vendored
@ -1 +1 @@
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Subproject commit ae9397c3b4e689a487fdd4b1425af5f519d3ea82
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Subproject commit 0e1ca91313e4b6ba3ea042b6378c3ff483781fb1
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@ -327,6 +327,8 @@ double precision function get_ao_two_e_integral(i,j,k,l,map) result(result)
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implicit none
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BEGIN_DOC
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! Gets one AO bi-electronic integral from the AO map
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!
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! i,j,k,l in physicist notation <ij|kl>
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END_DOC
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integer, intent(in) :: i,j,k,l
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integer(key_kind) :: idx
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@ -38,7 +38,7 @@ subroutine print_basis_correction
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write(*, '(A29,X,I3,X,A3,X,F16.10)') ' ECMD PBE-UEG , state ',istate,' = ',ecmd_pbe_ueg_mu_of_r(istate)
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enddo
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else if(mu_of_r_potential.EQ."cas_ful")then
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else if(mu_of_r_potential.EQ."cas_ful".or.mu_of_r_potential.EQ."cas_truncated".or.mu_of_r_potential.EQ."pure_act")then
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print*, ''
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print*,'Using a CAS-like two-body density to define mu(r)'
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print*,'This assumes that the CAS is a qualitative representation of the wave function '
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@ -262,17 +262,48 @@ subroutine set_natural_mos
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iorb = list_virt(i)
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do j = 1, n_core_inact_act_orb
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jorb = list_core_inact_act(j)
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if(one_e_dm_mo(iorb,jorb).ne. 0.d0)then
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print*,'AHAHAH'
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print*,iorb,jorb,one_e_dm_mo(iorb,jorb)
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stop
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endif
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enddo
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enddo
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call mo_as_svd_vectors_of_mo_matrix_eig(one_e_dm_mo,size(one_e_dm_mo,1),mo_num,mo_num,mo_occ,label)
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soft_touch mo_occ
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end
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subroutine set_natorb_no_ov_rot
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implicit none
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BEGIN_DOC
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! Set natural orbitals, obtained by diagonalization of the one-body density matrix
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! in the |MO| basis
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END_DOC
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character*(64) :: label
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double precision, allocatable :: tmp(:,:)
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allocate(tmp(mo_num, mo_num))
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label = "Natural"
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tmp = one_e_dm_mo
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integer :: i,j,iorb,jorb
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do i = 1, n_virt_orb
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iorb = list_virt(i)
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do j = 1, n_core_inact_act_orb
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jorb = list_core_inact_act(j)
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tmp(iorb, jorb) = 0.d0
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tmp(jorb, iorb) = 0.d0
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enddo
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enddo
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call mo_as_svd_vectors_of_mo_matrix_eig(tmp,size(tmp,1),mo_num,mo_num,mo_occ,label)
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soft_touch mo_occ
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end
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subroutine save_natural_mos_no_ov_rot
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implicit none
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BEGIN_DOC
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! Save natural orbitals, obtained by diagonalization of the one-body density matrix in
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! the |MO| basis
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END_DOC
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call set_natorb_no_ov_rot
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call nullify_small_elements(ao_num,mo_num,mo_coef,size(mo_coef,1),1.d-10)
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call orthonormalize_mos
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call save_mos
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end
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subroutine save_natural_mos
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implicit none
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BEGIN_DOC
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@ -384,6 +415,14 @@ END_PROVIDER
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END_PROVIDER
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BEGIN_PROVIDER [ double precision, one_e_dm_ao, (ao_num, ao_num)]
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implicit none
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BEGIN_DOC
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! one_e_dm_ao = one_e_dm_ao_alpha + one_e_dm_ao_beta
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END_DOC
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one_e_dm_ao = one_e_dm_ao_alpha + one_e_dm_ao_beta
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END_PROVIDER
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subroutine get_occupation_from_dets(istate,occupation)
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implicit none
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@ -37,13 +37,15 @@ double precision function g0_UEG_mu_inf(rho_a,rho_b)
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rs = (3d0 / (4d0*pi*rho))**(1d0/3d0) ! JT: serious bug fixed 20/03/19
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x = -d2*rs
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if(dabs(x).lt.50.d0)then
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g0_UEG_mu_inf= 0.5d0 * (1d0- B*rs + C*rs**2 + D*rs**3 + E*rs**4)*dexp(x)
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! g0_UEG_mu_inf= 0.5d0 * (1d0- B*rs + C*rs**2 + D*rs**3 + E*rs**4)*dexp(x)
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g0_UEG_mu_inf= 0.5d0 * (1d0+ rs* (-B + rs*(C + rs*(D + rs*E))))*dexp(x)
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else
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g0_UEG_mu_inf= 0.d0
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endif
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else
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g0_UEG_mu_inf= 0.d0
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endif
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g0_UEG_mu_inf = max(g0_UEG_mu_inf,1.d-14)
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end
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@ -6,7 +6,7 @@ size: (becke_numerical_grid.n_points_final_grid,determinants.n_states)
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[mu_of_r_potential]
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type: character*(32)
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doc: type of potential for the mu(r) interaction: can be [ hf| cas_ful | cas_truncated]
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doc: type of potential for the mu(r) interaction: can be [ hf| cas_ful | cas_truncated | pure_act]
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interface: ezfio, provider, ocaml
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default: hf
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@ -76,7 +76,11 @@ BEGIN_PROVIDER [integer, n_basis_orb]
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!
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! It corresponds to all MOs except those defined as "deleted"
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END_DOC
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n_basis_orb = n_all_but_del_orb
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if(mu_of_r_potential == "pure_act")then
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n_basis_orb = n_act_orb
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else
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n_basis_orb = n_all_but_del_orb
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endif
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END_PROVIDER
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BEGIN_PROVIDER [integer, list_basis, (n_basis_orb)]
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@ -89,9 +93,15 @@ BEGIN_PROVIDER [integer, list_basis, (n_basis_orb)]
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! It corresponds to all MOs except those defined as "deleted"
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END_DOC
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integer :: i
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do i = 1, n_all_but_del_orb
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list_basis(i) = list_all_but_del_orb(i)
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enddo
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if(mu_of_r_potential == "pure_act")then
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do i = 1, n_act_orb
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list_basis(i) = list_act(i)
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enddo
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else
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do i = 1, n_all_but_del_orb
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list_basis(i) = list_all_but_del_orb(i)
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enddo
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endif
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END_PROVIDER
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BEGIN_PROVIDER [double precision, basis_mos_in_r_array, (n_basis_orb,n_points_final_grid)]
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do ipoint = 1, n_points_final_grid
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if(mu_of_r_potential.EQ."hf")then
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mu_of_r_prov(ipoint,istate) = mu_of_r_hf(ipoint)
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else if(mu_of_r_potential.EQ."cas_ful".or.mu_of_r_potential.EQ."cas_truncated")then
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else if(mu_of_r_potential.EQ."cas_ful".or.mu_of_r_potential.EQ."cas_truncated".or.mu_of_r_potential.EQ."pure_act")then
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mu_of_r_prov(ipoint,istate) = mu_of_r_psi_cas(ipoint,istate)
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else
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print*,'you requested the following mu_of_r_potential'
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25
src/tools/save_natorb_no_ov_rot.irp.f
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25
src/tools/save_natorb_no_ov_rot.irp.f
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program save_natorb
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implicit none
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BEGIN_DOC
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! Save natural |MOs| into the |EZFIO|.
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!
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! This program reads the wave function stored in the |EZFIO| directory,
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! extracts the corresponding natural orbitals and setd them as the new
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! |MOs|.
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!
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! If this is a multi-state calculation, the density matrix that produces
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! the natural orbitals is obtained from an average of the density
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! matrices of each state with the corresponding
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! :option:`determinants state_average_weight`
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END_DOC
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read_wf = .True.
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touch read_wf
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call save_natural_mos_no_ov_rot
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call save_ref_determinant
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call ezfio_set_mo_two_e_ints_io_mo_two_e_integrals('None')
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call ezfio_set_mo_one_e_ints_io_mo_one_e_integrals('None')
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call ezfio_set_mo_one_e_ints_io_mo_integrals_kinetic('None')
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call ezfio_set_mo_one_e_ints_io_mo_integrals_n_e('None')
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call ezfio_set_mo_one_e_ints_io_mo_integrals_pseudo('None')
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end
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