Efficient Excitations and Spectra within a Perturbative Renormalization Approach

We present a self-consistent approach for computing the correlated quasiparticle spectrum of charged excitations in iterative O [ N 5 ] computational time. This is based on the auxiliary second-order Green’s function approach [ Backhouse, O. J. Chem. Theory Comput., 2000 ], in which a self-consisten...

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Published inJournal of chemical theory and computation Vol. 16; no. 10; pp. 6294 - 6304
Main Authors Backhouse, Oliver J, Booth, George H
Format Journal Article
LanguageEnglish
Published Washington American Chemical Society 13.10.2020
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ISSN1549-9618
1549-9626
1549-9626
DOI10.1021/acs.jctc.0c00701

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Summary:We present a self-consistent approach for computing the correlated quasiparticle spectrum of charged excitations in iterative O [ N 5 ] computational time. This is based on the auxiliary second-order Green’s function approach [ Backhouse, O. J. Chem. Theory Comput., 2000 ], in which a self-consistent effective Hamiltonian is constructed by systematically renormalizing the dynamical effects of the self-energy at second-order perturbation theory. From extensive benchmarking across the W4-11 molecular test set, we show that the iterative renormalization and truncation of the effective dynamical resolution arising from the 2h1p and 1h2p spaces can substantially improve the quality of the resulting ionization potential and electron affinity predictions compared to benchmark values. The resulting method is shown to be superior in accuracy to similarly scaling quantum chemical methods for charged excitations in EOM-CC2 and ADC(2), across this test set, while the self-consistency also removes the dependence on the underlying mean-field reference. The approach also allows for single-shot computation of the entire quasiparticle spectrum, which is applied to the benzoquinone molecule and demonstrates the reduction in the single-particle gap due to the correlated physics, and gives direct access to the localization of the Dyson orbitals.
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ISSN:1549-9618
1549-9626
1549-9626
DOI:10.1021/acs.jctc.0c00701