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891 lines
35 KiB
ReStructuredText
Needed Modules
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==============
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.. Do not edit this section It was auto-generated
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.. by the `update_README.py` script.
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.. image:: tree_dependency.png
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* `Integrals_Monoelec <http://github.com/LCPQ/quantum_package/tree/master/src/Integrals_Monoelec>`_
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* `Integrals_Bielec <http://github.com/LCPQ/quantum_package/tree/master/src/Integrals_Bielec>`_
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Documentation
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=============
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.. Do not edit this section It was auto-generated
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.. by the `update_README.py` script.
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`a_operator <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L1421>`_
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Needed for diag_H_mat_elem
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`abs_psi_coef_max <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L431>`_
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Max and min values of the coefficients
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`abs_psi_coef_min <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L432>`_
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Max and min values of the coefficients
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`ac_operator <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L1467>`_
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Needed for diag_H_mat_elem
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`apply_excitation <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L747>`_
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Undocumented
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`apply_hole <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L877>`_
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Undocumented
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`apply_holes <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L827>`_
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Undocumented
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`apply_mono <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/excitations_utils.irp.f#L1>`_
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Undocumented
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`apply_particle <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L855>`_
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Undocumented
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`apply_particles <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L798>`_
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Undocumented
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`bi_elec_ref_bitmask_energy <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ref_bitmask.irp.f#L5>`_
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Energy of the reference bitmask used in Slater rules
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`bitstring_to_list_ab <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L422>`_
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Gives the inidices(+1) of the bits set to 1 in the bit string
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For alpha/beta determinants
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`bitstring_to_list_ab_old <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L460>`_
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Gives the inidices(+1) of the bits set to 1 in the bit string
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For alpha/beta determinants
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`build_fock_tmp <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/Fock_diag.irp.f#L1>`_
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Build the diagonal of the Fock matrix corresponding to a generator
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determinant. F_00 is <i|H|i> = E0.
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`cisd <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/truncate_wf.irp.f#L1>`_
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Undocumented
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`connected_to_ref <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/connected_to_ref.irp.f#L245>`_
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Undocumented
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`connected_to_ref_by_mono <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/connected_to_ref.irp.f#L345>`_
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Undocumented
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`copy_h_apply_buffer_to_wf <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/H_apply.irp.f#L112>`_
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Copies the H_apply buffer to psi_coef.
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After calling this subroutine, N_det, psi_det and psi_coef need to be touched
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`create_microlist <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/filter_connected.irp.f#L131>`_
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Undocumented
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`create_minilist <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L807>`_
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Undocumented
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`create_minilist_find_previous <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L862>`_
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Undocumented
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`create_wf_of_psi_bilinear_matrix <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/spindeterminants.irp.f#L445>`_
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Generate a wave function containing all possible products
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of alpha and beta determinants
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`decode_exc <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L76>`_
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Decodes the exc arrays returned by get_excitation.
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h1,h2 : Holes
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p1,p2 : Particles
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s1,s2 : Spins (1:alpha, 2:beta)
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degree : Degree of excitation
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`decode_exc_int2 <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L142>`_
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Decodes the exc arrays returned by get_excitation.
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h1,h2 : Holes
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p1,p2 : Particles
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s1,s2 : Spins (1:alpha, 2:beta)
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degree : Degree of excitation
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`det_alpha_norm <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/spindeterminants.irp.f#L353>`_
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Norm of the alpha and beta spin determinants in the wave function:
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.br
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||Da||_i \sum_j C_{ij}**2
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`det_beta_norm <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/spindeterminants.irp.f#L354>`_
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Norm of the alpha and beta spin determinants in the wave function:
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.br
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||Da||_i \sum_j C_{ij}**2
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`det_coef <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ezfio_interface.irp.f#L120>`_
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det_coef
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`det_occ <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ezfio_interface.irp.f#L178>`_
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det_occ
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`det_search_key <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/connected_to_ref.irp.f#L1>`_
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Return an integer*8 corresponding to a determinant index for searching
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`det_to_occ_pattern <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/occ_pattern.irp.f#L2>`_
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Transform a determinant to an occupation pattern
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`detcmp <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L723>`_
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Undocumented
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`deteq <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L706>`_
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Undocumented
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`diag_algorithm <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L3>`_
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Diagonalization algorithm (Davidson or Lapack)
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`diag_h_mat_elem <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L1359>`_
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Computes <i|H|i>
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`diag_h_mat_elem_fock <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L1290>`_
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Computes <i|H|i> when i is at most a double excitation from
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a reference.
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`diagonalize_s2_betweenstates <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/s2.irp.f#L302>`_
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You enter with nstates vectors in u_0 that may be coupled by S^2
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The subroutine diagonalize the S^2 operator in the basis of these states.
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The vectors that you obtain in output are no more coupled by S^2,
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which does not necessary mean that they are eigenfunction of S^2.
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n,nmax,nstates = number of determinants, physical dimension of the arrays and number of states
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keys_tmp = array of integer(bit_kind) that represents the determinants
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psi_coefs(i,j) = coeff of the ith determinant in the jth state
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VECTORS ARE SUPPOSED TO BE ORTHONORMAL IN INPUT
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`do_mono_excitation <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/create_excitations.irp.f#L1>`_
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Apply the mono excitation operator : a^{dager}_(i_particle) a_(i_hole) of spin = ispin
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on key_in
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ispin = 1 == alpha
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ispin = 2 == beta
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i_ok = 1 == the excitation is possible
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i_ok = -1 == the excitation is not possible
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`double_exc_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants_bitmasks.irp.f#L40>`_
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double_exc_bitmask(:,1,i) is the bitmask for holes of excitation 1
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double_exc_bitmask(:,2,i) is the bitmask for particles of excitation 1
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double_exc_bitmask(:,3,i) is the bitmask for holes of excitation 2
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double_exc_bitmask(:,4,i) is the bitmask for particles of excitation 2
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for a given couple of hole/particle excitations i.
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`doubly_occ_empty_in_couple <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/usefull_for_ovb.irp.f#L41>`_
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n_couples is the number of couples of orbitals to be checked
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couples(i,1) = first orbital of the ith couple
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couples(i,2) = second orbital of the ith couple
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returns the array couples_out
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couples_out(i) = .True. if det_in contains
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an orbital empty in the ith couple AND
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an orbital doubly occupied in the ith couple
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`doubly_occ_empty_in_couple_and_no_hund_elsewhere <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/usefull_for_ovb.irp.f#L135>`_
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n_couples is the number of couples of orbitals to be checked
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couples(i,1) = first orbital of the ith couple
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couples(i,2) = second orbital of the ith couple
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returns the array couples_out
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couples_out(i) = .True. if det_in contains
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an orbital empty in the ith couple AND
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an orbital doubly occupied in the ith couple
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`expected_s2 <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/s2.irp.f#L48>`_
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Expected value of S2 : S*(S+1)
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`fill_h_apply_buffer_no_selection <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/H_apply.irp.f#L264>`_
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Fill the H_apply buffer with determiants for CISD
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`filter_connected <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/filter_connected.irp.f#L2>`_
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Filters out the determinants that are not connected by H
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.br
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returns the array idx which contains the index of the
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.br
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determinants in the array key1 that interact
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.br
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via the H operator with key2.
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.br
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idx(0) is the number of determinants that interact with key1
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`filter_connected_i_h_psi0 <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/filter_connected.irp.f#L232>`_
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returns the array idx which contains the index of the
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.br
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determinants in the array key1 that interact
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.br
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via the H operator with key2.
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.br
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idx(0) is the number of determinants that interact with key1
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`filter_connected_i_h_psi0_sc2 <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/filter_connected.irp.f#L326>`_
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standard filter_connected_i_H_psi but returns in addition
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.br
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the array of the index of the non connected determinants to key1
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.br
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in order to know what double excitation can be repeated on key1
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.br
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idx_repeat(0) is the number of determinants that can be used
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.br
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to repeat the excitations
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`flip_generators <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L354>`_
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Undocumented
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`generate_all_alpha_beta_det_products <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/spindeterminants.irp.f#L503>`_
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Create a wave function from all possible alpha x beta determinants
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`get_double_excitation <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L208>`_
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Returns the two excitation operators between two doubly excited determinants and the phase
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`get_double_excitation_phase <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L1530>`_
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Undocumented
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`get_excitation <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L30>`_
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Returns the excitation operators between two determinants and the phase
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`get_excitation_degree <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L1>`_
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Returns the excitation degree between two determinants
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`get_excitation_degree_vector <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L1200>`_
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Applies get_excitation_degree to an array of determinants
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`get_index_in_psi_det_alpha_unique <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/spindeterminants.irp.f#L141>`_
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Returns the index of the determinant in the ``psi_det_alpha_unique`` array
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`get_index_in_psi_det_beta_unique <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/spindeterminants.irp.f#L223>`_
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Returns the index of the determinant in the ``psi_det_beta_unique`` array
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`get_index_in_psi_det_sorted_bit <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/connected_to_ref.irp.f#L50>`_
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Returns the index of the determinant in the ``psi_det_sorted_bit`` array
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`get_mono_excitation <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L343>`_
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Returns the excitation operator between two singly excited determinants and the phase
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`get_occ_from_key <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L1513>`_
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Returns a list of occupation numbers from a bitstring
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`get_phase <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L1627>`_
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Returns the phase between key1 and key2
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`get_s2 <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/s2.irp.f#L1>`_
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Returns <S^2>
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`get_uj_s2_ui <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/s2.irp.f#L253>`_
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returns the matrix elements of S^2 "s2(i,j)" between the "nstates" states
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psi_coefs_tmp(:,i) and psi_coefs_tmp(:,j)
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`getmobiles <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/filter_connected.irp.f#L101>`_
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Undocumented
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`give_index_of_doubly_occ_in_active_space <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/usefull_for_ovb.irp.f#L97>`_
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Undocumented
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`h_apply_buffer_allocated <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/H_apply.irp.f#L15>`_
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Buffer of determinants/coefficients/perturbative energy for H_apply.
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Uninitialized. Filled by H_apply subroutines.
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`h_apply_buffer_lock <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/H_apply.irp.f#L16>`_
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Buffer of determinants/coefficients/perturbative energy for H_apply.
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Uninitialized. Filled by H_apply subroutines.
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`h_matrix_all_dets <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/utils.irp.f#L1>`_
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H matrix on the basis of the slater determinants defined by psi_det
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`h_matrix_cas <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/psi_cas.irp.f#L115>`_
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Undocumented
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`i_h_j <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L500>`_
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Returns <i|H|j> where i and j are determinants
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`i_h_j_phase_out <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L602>`_
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Returns <i|H|j> where i and j are determinants
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`i_h_j_verbose <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L704>`_
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Returns <i|H|j> where i and j are determinants
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`i_h_psi <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L938>`_
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Computes <i|H|Psi> = \sum_J c_J <i|H|J>.
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.br
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Uses filter_connected_i_H_psi0 to get all the |J> to which |i>
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is connected.
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The i_H_psi_minilist is much faster but requires to build the
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minilists
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`i_h_psi_minilist <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L994>`_
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Computes <i|H|Psi> = \sum_J c_J <i|H|J>.
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.br
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Uses filter_connected_i_H_psi0 to get all the |J> to which |i>
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is connected. The |J> are searched in short pre-computed lists.
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`i_h_psi_sc2 <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L1097>`_
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<key|H|psi> for the various Nstate
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.br
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returns in addition
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.br
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the array of the index of the non connected determinants to key1
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.br
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in order to know what double excitation can be repeated on key1
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.br
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idx_repeat(0) is the number of determinants that can be used
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.br
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to repeat the excitations
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`i_h_psi_sc2_verbose <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L1144>`_
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<key|H|psi> for the various Nstate
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.br
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returns in addition
|
|
.br
|
|
the array of the index of the non connected determinants to key1
|
|
.br
|
|
in order to know what double excitation can be repeated on key1
|
|
.br
|
|
idx_repeat(0) is the number of determinants that can be used
|
|
.br
|
|
to repeat the excitations
|
|
|
|
|
|
`i_h_psi_sec_ord <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/slater_rules.irp.f#L1050>`_
|
|
<key|H|psi> for the various Nstates
|
|
|
|
|
|
`i_s2_psi_minilist <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/s2.irp.f#L421>`_
|
|
Computes <i|S2|Psi> = \sum_J c_J <i|S2|J>.
|
|
.br
|
|
Uses filter_connected_i_H_psi0 to get all the |J> to which |i>
|
|
is connected. The |J> are searched in short pre-computed lists.
|
|
|
|
|
|
`idx_cas <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/psi_cas.irp.f#L5>`_
|
|
CAS wave function, defined from the application of the CAS bitmask on the
|
|
determinants. idx_cas gives the indice of the CAS determinant in psi_det.
|
|
|
|
|
|
`idx_non_cas <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/psi_cas.irp.f#L65>`_
|
|
Set of determinants which are not part of the CAS, defined from the application
|
|
of the CAS bitmask on the determinants.
|
|
idx_non_cas gives the indice of the determinant in psi_det.
|
|
|
|
|
|
`is_connected_to <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/connected_to_ref.irp.f#L157>`_
|
|
Undocumented
|
|
|
|
|
|
`is_connected_to_by_mono <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/connected_to_ref.irp.f#L212>`_
|
|
Undocumented
|
|
|
|
|
|
`is_generable_cassd <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/connected_to_ref.irp.f#L191>`_
|
|
Undocumented
|
|
|
|
|
|
`is_in_wavefunction <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/connected_to_ref.irp.f#L36>`_
|
|
True if the determinant ``det`` is in the wave function
|
|
|
|
|
|
`kinetic_ref_bitmask_energy <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ref_bitmask.irp.f#L3>`_
|
|
Energy of the reference bitmask used in Slater rules
|
|
|
|
|
|
`make_s2_eigenfunction <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/occ_pattern.irp.f#L251>`_
|
|
Undocumented
|
|
|
|
|
|
`max_degree_exc <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L50>`_
|
|
Maximum degree of excitation in the wf
|
|
|
|
|
|
`mono_elec_ref_bitmask_energy <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ref_bitmask.irp.f#L2>`_
|
|
Energy of the reference bitmask used in Slater rules
|
|
|
|
|
|
`n_closed_shell <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/usefull_for_ovb.irp.f#L13>`_
|
|
Undocumented
|
|
|
|
|
|
`n_closed_shell_cas <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/usefull_for_ovb.irp.f#L24>`_
|
|
Undocumented
|
|
|
|
|
|
`n_det <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L20>`_
|
|
Number of determinants in the wave function
|
|
|
|
|
|
`n_det_alpha_unique <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/spindeterminants.irp.f_template_136#L4>`_
|
|
Unique alpha determinants
|
|
|
|
|
|
`n_det_beta_unique <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/spindeterminants.irp.f_template_136#L80>`_
|
|
Unique beta determinants
|
|
|
|
|
|
`n_det_cas <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/psi_cas.irp.f#L6>`_
|
|
CAS wave function, defined from the application of the CAS bitmask on the
|
|
determinants. idx_cas gives the indice of the CAS determinant in psi_det.
|
|
|
|
|
|
`n_det_max <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ezfio_interface.irp.f#L44>`_
|
|
Max number of determinants in the wave function
|
|
|
|
|
|
`n_det_max_jacobi <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ezfio_interface.irp.f#L82>`_
|
|
Maximum number of determinants diagonalized by Jacobi
|
|
|
|
|
|
`n_det_max_property <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ezfio_interface.irp.f#L236>`_
|
|
Max number of determinants in the wave function when you select for a given property
|
|
|
|
|
|
`n_det_non_cas <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/psi_cas.irp.f#L66>`_
|
|
Set of determinants which are not part of the CAS, defined from the application
|
|
of the CAS bitmask on the determinants.
|
|
idx_non_cas gives the indice of the determinant in psi_det.
|
|
|
|
|
|
`n_double_exc_bitmasks <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants_bitmasks.irp.f#L31>`_
|
|
Number of double excitation bitmasks
|
|
|
|
|
|
`n_occ_pattern <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/occ_pattern.irp.f#L143>`_
|
|
array of the occ_pattern present in the wf
|
|
psi_occ_pattern(:,1,j) = jth occ_pattern of the wave function : represent all the single occupation
|
|
psi_occ_pattern(:,2,j) = jth occ_pattern of the wave function : represent all the double occupation
|
|
|
|
|
|
`n_open_shell <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/usefull_for_ovb.irp.f#L2>`_
|
|
Undocumented
|
|
|
|
|
|
`n_single_exc_bitmasks <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants_bitmasks.irp.f#L8>`_
|
|
Number of single excitation bitmasks
|
|
|
|
|
|
`n_states <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ezfio_interface.irp.f#L63>`_
|
|
Number of states to consider
|
|
|
|
|
|
`neutral_no_hund_in_couple <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/usefull_for_ovb.irp.f#L220>`_
|
|
n_couples is the number of couples of orbitals to be checked
|
|
couples(i,1) = first orbital of the ith couple
|
|
couples(i,2) = second orbital of the ith couple
|
|
returns the array couples_out
|
|
couples_out(i) = .True. if det_in contains
|
|
an orbital empty in the ith couple AND
|
|
an orbital doubly occupied in the ith couple
|
|
|
|
|
|
`nucl_elec_ref_bitmask_energy <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ref_bitmask.irp.f#L4>`_
|
|
Energy of the reference bitmask used in Slater rules
|
|
|
|
|
|
`occ_pattern_search_key <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/connected_to_ref.irp.f#L18>`_
|
|
Return an integer*8 corresponding to a determinant index for searching
|
|
|
|
|
|
`occ_pattern_to_dets <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/occ_pattern.irp.f#L42>`_
|
|
Generate all possible determinants for a give occ_pattern
|
|
|
|
|
|
`occ_pattern_to_dets_size <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/occ_pattern.irp.f#L20>`_
|
|
Number of possible determinants for a given occ_pattern
|
|
|
|
|
|
`one_body_dm_ao_alpha <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/density_matrix.irp.f#L234>`_
|
|
one body density matrix on the AO basis : rho_AO(alpha) , rho_AO(beta)
|
|
|
|
|
|
`one_body_dm_ao_beta <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/density_matrix.irp.f#L235>`_
|
|
one body density matrix on the AO basis : rho_AO(alpha) , rho_AO(beta)
|
|
|
|
|
|
`one_body_dm_mo <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/density_matrix.irp.f#L161>`_
|
|
One-body density matrix
|
|
|
|
|
|
`one_body_dm_mo_alpha <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/density_matrix.irp.f#L1>`_
|
|
Alpha and beta one-body density matrix for each state
|
|
|
|
|
|
`one_body_dm_mo_beta <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/density_matrix.irp.f#L2>`_
|
|
Alpha and beta one-body density matrix for each state
|
|
|
|
|
|
`one_body_single_double_dm_mo_alpha <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/density_matrix.irp.f#L78>`_
|
|
Alpha and beta one-body density matrix for each state
|
|
|
|
|
|
`one_body_single_double_dm_mo_beta <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/density_matrix.irp.f#L79>`_
|
|
Alpha and beta one-body density matrix for each state
|
|
|
|
|
|
`one_body_spin_density_ao <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/density_matrix.irp.f#L210>`_
|
|
one body spin density matrix on the AO basis : rho_AO(alpha) - rho_AO(beta)
|
|
|
|
|
|
`one_body_spin_density_mo <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/density_matrix.irp.f#L169>`_
|
|
rho(alpha) - rho(beta)
|
|
|
|
|
|
`only_single_double_dm <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ezfio_interface.irp.f#L159>`_
|
|
If true, The One body DM is calculated with ignoring the Double<->Doubles extra diag elements
|
|
|
|
|
|
`psi_average_norm_contrib <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L292>`_
|
|
Contribution of determinants to the state-averaged density
|
|
|
|
|
|
`psi_average_norm_contrib_sorted <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L326>`_
|
|
Wave function sorted by determinants contribution to the norm (state-averaged)
|
|
|
|
|
|
`psi_bilinear_matrix <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/spindeterminants.irp.f#L428>`_
|
|
Coefficient matrix if the wave function is expressed in a bilinear form :
|
|
D_a^t C D_b
|
|
|
|
|
|
`psi_bilinear_matrix_columns <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/spindeterminants.irp.f#L390>`_
|
|
Sparse coefficient matrix if the wave function is expressed in a bilinear form :
|
|
D_a^t C D_b
|
|
|
|
|
|
`psi_bilinear_matrix_rows <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/spindeterminants.irp.f#L389>`_
|
|
Sparse coefficient matrix if the wave function is expressed in a bilinear form :
|
|
D_a^t C D_b
|
|
|
|
|
|
`psi_bilinear_matrix_values <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/spindeterminants.irp.f#L388>`_
|
|
Sparse coefficient matrix if the wave function is expressed in a bilinear form :
|
|
D_a^t C D_b
|
|
|
|
|
|
`psi_cas <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/psi_cas.irp.f#L3>`_
|
|
CAS wave function, defined from the application of the CAS bitmask on the
|
|
determinants. idx_cas gives the indice of the CAS determinant in psi_det.
|
|
|
|
|
|
`psi_cas_coef <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/psi_cas.irp.f#L4>`_
|
|
CAS wave function, defined from the application of the CAS bitmask on the
|
|
determinants. idx_cas gives the indice of the CAS determinant in psi_det.
|
|
|
|
|
|
`psi_cas_coef_sorted_bit <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/psi_cas.irp.f#L50>`_
|
|
CAS determinants sorted to accelerate the search of a random determinant in the wave
|
|
function.
|
|
|
|
|
|
`psi_cas_energy <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/psi_cas.irp.f#L146>`_
|
|
Undocumented
|
|
|
|
|
|
`psi_cas_energy_diagonalized <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/psi_cas.irp.f#L128>`_
|
|
Undocumented
|
|
|
|
|
|
`psi_cas_sorted_bit <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/psi_cas.irp.f#L49>`_
|
|
CAS determinants sorted to accelerate the search of a random determinant in the wave
|
|
function.
|
|
|
|
|
|
`psi_coef <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L246>`_
|
|
The wave function coefficients. Initialized with Hartree-Fock if the EZFIO file
|
|
is empty
|
|
|
|
|
|
`psi_coef_cas_diagonalized <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/psi_cas.irp.f#L127>`_
|
|
Undocumented
|
|
|
|
|
|
`psi_coef_max <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L429>`_
|
|
Max and min values of the coefficients
|
|
|
|
|
|
`psi_coef_min <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L430>`_
|
|
Max and min values of the coefficients
|
|
|
|
|
|
`psi_coef_sorted <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L325>`_
|
|
Wave function sorted by determinants contribution to the norm (state-averaged)
|
|
|
|
|
|
`psi_coef_sorted_bit <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L373>`_
|
|
Determinants on which we apply <i|H|psi> for perturbation.
|
|
They are sorted by determinants interpreted as integers. Useful
|
|
to accelerate the search of a random determinant in the wave
|
|
function.
|
|
|
|
|
|
`psi_det <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L83>`_
|
|
The wave function determinants. Initialized with Hartree-Fock if the EZFIO file
|
|
is empty
|
|
|
|
|
|
`psi_det_alpha <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/spindeterminants.irp.f#L27>`_
|
|
List of alpha determinants of psi_det
|
|
|
|
|
|
`psi_det_alpha_unique <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/spindeterminants.irp.f_template_136#L3>`_
|
|
Unique alpha determinants
|
|
|
|
|
|
`psi_det_beta <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/spindeterminants.irp.f#L41>`_
|
|
List of beta determinants of psi_det
|
|
|
|
|
|
`psi_det_beta_unique <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/spindeterminants.irp.f_template_136#L79>`_
|
|
Unique beta determinants
|
|
|
|
|
|
`psi_det_size <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L65>`_
|
|
Size of the psi_det/psi_coef arrays
|
|
|
|
|
|
`psi_det_sorted <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L324>`_
|
|
Wave function sorted by determinants contribution to the norm (state-averaged)
|
|
|
|
|
|
`psi_det_sorted_bit <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L372>`_
|
|
Determinants on which we apply <i|H|psi> for perturbation.
|
|
They are sorted by determinants interpreted as integers. Useful
|
|
to accelerate the search of a random determinant in the wave
|
|
function.
|
|
|
|
|
|
`psi_non_cas <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/psi_cas.irp.f#L63>`_
|
|
Set of determinants which are not part of the CAS, defined from the application
|
|
of the CAS bitmask on the determinants.
|
|
idx_non_cas gives the indice of the determinant in psi_det.
|
|
|
|
|
|
`psi_non_cas_coef <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/psi_cas.irp.f#L64>`_
|
|
Set of determinants which are not part of the CAS, defined from the application
|
|
of the CAS bitmask on the determinants.
|
|
idx_non_cas gives the indice of the determinant in psi_det.
|
|
|
|
|
|
`psi_non_cas_coef_sorted_bit <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/psi_cas.irp.f#L103>`_
|
|
CAS determinants sorted to accelerate the search of a random determinant in the wave
|
|
function.
|
|
|
|
|
|
`psi_non_cas_sorted_bit <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/psi_cas.irp.f#L102>`_
|
|
CAS determinants sorted to accelerate the search of a random determinant in the wave
|
|
function.
|
|
|
|
|
|
`psi_occ_pattern <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/occ_pattern.irp.f#L142>`_
|
|
array of the occ_pattern present in the wf
|
|
psi_occ_pattern(:,1,j) = jth occ_pattern of the wave function : represent all the single occupation
|
|
psi_occ_pattern(:,2,j) = jth occ_pattern of the wave function : represent all the double occupation
|
|
|
|
|
|
`pull_pt2 <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/H_apply.irp.f#L364>`_
|
|
Pull PT2 calculation in the collector
|
|
|
|
|
|
`push_pt2 <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/H_apply.irp.f#L307>`_
|
|
Push PT2 calculation to the collector
|
|
|
|
|
|
`put_gess <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/guess_triplet.irp.f#L1>`_
|
|
Undocumented
|
|
|
|
|
|
`read_dets <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L454>`_
|
|
Reads the determinants from the EZFIO file
|
|
|
|
|
|
`read_wf <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ezfio_interface.irp.f#L101>`_
|
|
If true, read the wave function from the EZFIO file
|
|
|
|
|
|
`rec_occ_pattern_to_dets <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/occ_pattern.irp.f#L102>`_
|
|
Undocumented
|
|
|
|
|
|
`ref_bitmask_energy <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ref_bitmask.irp.f#L1>`_
|
|
Energy of the reference bitmask used in Slater rules
|
|
|
|
|
|
`remove_duplicates_in_psi_det <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/H_apply.irp.f#L198>`_
|
|
Removes duplicate determinants in the wave function.
|
|
|
|
|
|
`resize_h_apply_buffer <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/H_apply.irp.f#L57>`_
|
|
Resizes the H_apply buffer of proc iproc. The buffer lock should
|
|
be set before calling this function.
|
|
|
|
|
|
`s2_eig <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ezfio_interface.irp.f#L198>`_
|
|
Force the wave function to be an eigenfunction of S^2
|
|
|
|
|
|
`s2_u_0 <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/s2.irp.f#L105>`_
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Computes v_0 = S^2|u_0>
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.br
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n : number of determinants
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.br
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`s2_u_0_nstates <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/s2.irp.f#L121>`_
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Computes v_0 = S^2|u_0>
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.br
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n : number of determinants
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.br
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`s2_values <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/s2.irp.f#L66>`_
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array of the averaged values of the S^2 operator on the various states
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`s_z <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/s2.irp.f#L36>`_
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z component of the Spin
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`s_z2_sz <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/s2.irp.f#L37>`_
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z component of the Spin
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`save_hf <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/save_HF_determinant.irp.f#L1>`_
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Undocumented
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`save_natorb <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/save_natorb.irp.f#L1>`_
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Undocumented
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`save_natural_mos <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/density_matrix.irp.f#L190>`_
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Save natural orbitals, obtained by diagonalization of the one-body density matrix in the MO basis
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`save_ref_determinant <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L500>`_
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Undocumented
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`save_wavefunction <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L511>`_
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Save the wave function into the EZFIO file
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`save_wavefunction_general <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L530>`_
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Save the wave function into the EZFIO file
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`save_wavefunction_specified <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L618>`_
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Save the wave function into the EZFIO file
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`save_wavefunction_unsorted <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L521>`_
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Save the wave function into the EZFIO file
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`set_bit_to_integer <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/create_excitations.irp.f#L38>`_
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Undocumented
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`set_natural_mos <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/density_matrix.irp.f#L177>`_
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Set natural orbitals, obtained by diagonalization of the one-body density matrix in the MO basis
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`single_exc_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants_bitmasks.irp.f#L17>`_
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single_exc_bitmask(:,1,i) is the bitmask for holes
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single_exc_bitmask(:,2,i) is the bitmask for particles
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for a given couple of hole/particle excitations i.
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`sort_dets_by_det_search_key <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/determinants.irp.f#L386>`_
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Determinants are sorted are sorted according to their det_search_key.
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Useful to accelerate the search of a random determinant in the wave
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function.
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`spin_det_search_key <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/spindeterminants.irp.f#L9>`_
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Return an integer(8) corresponding to a determinant index for searching
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`state_average_weight <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/density_matrix.irp.f#L201>`_
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Weights in the state-average calculation of the density matrix
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`target_energy <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ezfio_interface.irp.f#L140>`_
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Energy that should be obtained when truncating the wave function (optional)
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`threshold_generators <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ezfio_interface.irp.f#L217>`_
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Thresholds on generators (fraction of the norm)
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`threshold_selectors <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/ezfio_interface.irp.f#L6>`_
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Thresholds on selectors (fraction of the norm)
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`u_0_s2_u_0 <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/s2.irp.f#L78>`_
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Computes e_0 = <u_0|S2|u_0>/<u_0|u_0>
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.br
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n : number of determinants
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.br
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`write_spindeterminants <http://github.com/LCPQ/quantum_package/tree/master/src/Determinants/spindeterminants.irp.f#L305>`_
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Undocumented
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