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Restrictions: results not trustworthy for higher excited states
Users should be aware of another technical point: Excited states are usually
calculated from a Davidson diagonalization procedure, i.e., only a small
number of eigenvalues and eigenvectors describing the lowest excitations are
obtained. During finite displacements, some of the higher calculated states
might leave the calculated energy window, while others enter it. Hence, the
character of some of the higher calculated states can change. In such a case,
the numerical differentiation based on a (simple) diabatic pictures will fail
for the higher states, since no mapping between the excited states for
reference (equilibrium) and displaced structure can be carried out.
The solution is rather simple: Users should always ask for more excited states
than they are actually interested in, and discard the data for higher states,
in particular for those which could not successfully be mapped for displaced
structures (look for messages in the output like
'State No. X cannot be expressed in terms of reference states').
For advanced users it should be mentioned that it is possible to set an
energy window within the range of states calculated, and only the states
within this energy window will be taken into account in the evaluation.
See the subkey ELTHRESH and EUTHRESH of the block key VIBRON.
Furthermore, it is possible to pick out certain states from this energy
window, and only perform the mapping (and diabatization, if requested)
and differentiation for them.
See the subkey SELSTATE of the block key VIBRON.
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