2013
DOI: 10.1063/1.4795750
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Complex-scaled equation-of-motion coupled-cluster method with single and double substitutions for autoionizing excited states: Theory, implementation, and examples

Abstract: Theory and implementation of complex-scaled variant of equation-of-motion coupled-cluster method for excitation energies with single and double substitutions (EOM-EE-CCSD) is presented. The complex-scaling formalism extends the EOM-EE-CCSD model to resonance states, i.e., excited states that are metastable with respect to electron ejection. The method is applied to Feshbach resonances in atomic systems (He, H(-), and Be). The dependence of the results on one-electron basis set is quantified and analyzed. Energ… Show more

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Cited by 71 publications
(88 citation statements)
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“…By using complex scaling and complex absorbing potential techniques, we extended these powerful methods to describe autoionising states, such as transient anions, highly excited electronic states, and core-ionised species [183][184][185]. In addition, users can employ stabilisation techniques using charged sphere and scaled atomic charges options [186].…”
Section: Coupled Cluster Methodsmentioning
confidence: 99%
“…By using complex scaling and complex absorbing potential techniques, we extended these powerful methods to describe autoionising states, such as transient anions, highly excited electronic states, and core-ionised species [183][184][185]. In addition, users can employ stabilisation techniques using charged sphere and scaled atomic charges options [186].…”
Section: Coupled Cluster Methodsmentioning
confidence: 99%
“…(6) are square integrable. This feature makes it possible to use bound-state methods to solve (6), including configuration interaction [14,15], Faddeev and Faddeev-Yakubovsky [39,40], and the coupled cluster method [41]. Because the resonant states are square integrable, they can be normalized to one.…”
Section: B Complex-scaling Methodsmentioning
confidence: 99%
“…4,[18][19][20][21] The EOM-CC formalism [22][23][24][25][26][27] allows to treat electronically excited 24 (EOM-EE), ionized 28 (EOM-IP), and electron-attached 29 (EOM-EA) states as eigenfunctions of the same effective Hamiltonian, which is crucial for electronic resonances because it enables a consistent description of a resonance relative to the ionization and detachment continua. 30 Furthermore, EOM-CC treats states with different character on an equal footing and by including higher excitations in the ansatz for the wave function, the description can be systematically improved up to the full configuration interaction limit.…”
Section: Introductionmentioning
confidence: 99%