7.7 Non-Orthogonal Configuration Interaction with Single Substitutions (NOCIS) and Static Exchange (STEX)

7.7.1 NOCIS

(May 16, 2021)

The motivation for NOCIS 819 Oosterbaan K. J., White A. F., Head-Gordon M.
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, 820 Oosterbaan K. J., White A. F., Head-Gordon M.
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, 818 Oosterbaan K. J. et al.
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is the desire to improve on CIS while still maintaining a reasonably low computational scaling. It does so by including orbital relaxation, which CIS neglects altogether, and the non-orthogonal interaction between multiple core-hole references, such as the O 1s orbitals in O2.

A brief overview of the NOCIS algorithm is as follows: after a ground-state orbital optimization, a Maximum Overlap Method (MOM) 352 Gilbert A. T. B., Besley N. A., Gill P. M. W.
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is done for an ionization from each localized core orbital of interest. This introduces orbital relaxation, and also renders the excited states non-orthogonal to the ground state. The Hamiltonian, overlap, and total spin squared matrices are constructed using the Slater-Condon rules for matrix elements between determinants which share a common set of orbitals and NOCI for the remaining matrix elements 1088 Thom A. J. W., Head-Gordon M.
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(2009), 131, pp. 124113.
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. Finally, the generalized eigenvalue problem is solved.

A key feature in open-shell NOCIS is a separate optimization of any open-shell references, which are states in which a core-electron is excited to a singly-occupied ground-state orbital. These separate optimizations render these states non-orthogonal to the other excited states.

NOCIS is spin-pure, size consistent, and maintains spatial symmetry. Like CIS, NOCIS produces excited states with the same ms as the reference but potentially with larger total spin. For example, performing NOCIS on a molecule with a singlet ground state will produce both singlet and triplet excited states.