Aufbau Suppressed Coupled Cluster Theory for Doubly Excited States
Qasim Javed, Harrison Tuckman, Eric Neuscamman
TL;DR
This work extends Aufbau suppressed coupled cluster (ASCC) theory to doubly excited states by initializing the zeroth-order wavefunction to capture the dominant doubly excited configurations while preserving CCSD-like scaling ($O(N^6)$). It develops a perturbative, multi-space framework with a de-excitation operator to suppress the Aufbau determinant and carefully partitions the cluster operator into non-primary, mixed, and primary parts, enabling accurate 1-CSF and multi-CSF doubly excited states at CCSD-level cost. Across 1-CSF and 2-CSF tests, ASCC achieves excitation energies within roughly $0.15$–$0.30$ eV of benchmark references, substantially outperforming EOM-based approaches and rivaling higher-level CC methods in this challenging regime. The results demonstrate strong potential for applying ASCC to multi-configurational double excitations while highlighting open questions about generalizing to larger primary spaces and more complex multi-reference cases, with promising implications for photochemistry and spectroscopy.
Abstract
We generalize the Aufbau suppressed coupled cluster formalism into the realm of doubly excited states by deriving, implementing, and testing a wave function initialization strategy that allows the zeroth order wave function to match the largest configurations of a doubly excited reference wave function while maintaining the method's overall asymptotic cost parity with ground state singles and doubles theory. Starting from state-averaged complete active space self consistent field references, this approach produces highly accurate excitation energies for states dominated by a single doubly excited determinant, as well as states in glyoxal and similar molecules where two different doubly excited determinants have large weights. Typical excitation energy errors in both types of states are on the order of 0.15 eV, with the largest observed error being 0.3 eV. These errors stand in stark contrast to equation of motion methods, where typical errors are 4 to 6 eV at the singles and doubles level and 0.4 to 0.8 eV at the full triples level. It remains an open question how best to generalize the Aufbau suppression approach into an even wider variety of multi-configurational double excitations, but these early results offer strong motivation for further investigation.
