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QuantumPackage/docs/source/programs/cisd.rst

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2019-01-25 11:39:31 +01:00
.. _cisd:
.. program:: cisd
====
cisd
====
and performs all single and double excitations on top of it, disregarding
spatial symmetry and compute the "n_states" lowest eigenstates of that CI
matrix (see :option:`determinants n_states`).
This program can be useful in many cases:
* GROUND STATE CALCULATION: if even after a :c:func:`cis` calculation, natural
orbitals (see :c:func:`save_natorb`) and then :c:func:`scf` optimization, you are not sure to have the lowest scf
solution,
do the same strategy with the :c:func:`cisd` executable instead of the :c:func:`cis` exectuable to generate the natural
orbitals as a guess for the :c:func:`scf`.
* EXCITED STATES CALCULATIONS: the lowest excited states are much likely to
be dominanted by single- or double-excitations.
Therefore, running a :c:func:`cisd` will save the "n_states" lowest states within
the CISD space
in the EZFIO folder, which can afterward be used as guess wave functions
for a further multi-state fci calculation if you specify "read_wf" = True
before running the fci executable (see :option:`determinants read_wf`).
Also, if you specify "s2_eig" = True, the cisd will only retain states
having the good value :math:`S^2` value
(see :option:`determinants expected_s2` and :option:`determinants s2_eig`).
If "s2_eig" = False, it will take the lowest n_states, whatever
multiplicity they are.
Note: if you would like to discard some orbitals, use
:ref:`qp_set_mo_class` to specify:
* "core" orbitals which will be always doubly occupied
* "act" orbitals where an electron can be either excited from or to
* "del" orbitals which will be never occupied
Needs:
.. hlist::
:columns: 3
* :c:data:`read_wf`
Calls:
.. hlist::
:columns: 3
* :c:func:`run`
Touches:
.. hlist::
:columns: 3
* :c:data:`fock_matrix_ao_alpha`
* :c:data:`fock_matrix_ao_alpha`
* :c:data:`mo_coef`
* :c:data:`level_shift`
* :c:data:`mo_coef`
* :c:data:`read_wf`