posted on 2020-07-20, 17:14authored byAbhishek Khedkar, Michael Roemelt
Multireference
electronic structure methods based on the CAS (complete
active space) ansatz are well-established as a means to provide reliable
predictions of physical properties of strongly correlated systems.
A critical aspect of every CAS calculation is the selection of an
adequate active space, in particular as the boundaries for tractable
active spaces have been shifted significantly with the emergence of
efficient approximations to the Full-CI problem like the density matrix
renormalization group and full-CI quantum Monte Carlo. Recently, we
proposed an active space selection based on first-order perturbation
theory (ASS1ST) that yields satisfactory results for the electronic
ground state of a variety of strongly correlated systems. In this
work, we present a state-averaged extension of ASS1ST (SA-ASS1ST)
that determines suitable active spaces when electronically excited
states are targeted. Furthermore, the computational costs of the single
state and state-averaged variants are significantly reduced by a simple
approximation that avoids the most expensive step of the original
method, the evaluation of active space four-electron reduced density
matrices, altogether. After the applicability of the approximation
is established, test calculations on a biomimetic Mn4O4 cluster demonstrate the enhanced range of ASS1ST in terms
of system size and complexity. Furthermore, calculations on [VOCl4]2–, MeMn(CO)3-α-diimine,
and anthracene show that SA-ASS1ST suggests well-suited active spaces
to describe d → d and charge-transfer excitations in transition-metal
complexes as well as π → π* excitations in aryl
compounds. Finally, the application of ASS1ST on multiple points of
the potential energy surface of Cr2 illustrates the applicability
of the method even when extremely complicated bonding patterns are
met. More importantly, however, it highlights the necessity to use
special strategies when different points of a potential energy surface
are investigated, e.g., during chemical reactions.