2018
DOI: 10.1137/17m1116611
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Analysis of the Extended Coupled-Cluster Method in Quantum Chemistry

Abstract: The mathematical foundation of the so-called extended coupled-cluster method for the solution of the many-fermion Schrödinger equation is here developed. We prove an existence and uniqueness result, both in the full infinite-dimensional amplitude space as well as for discretized versions of it. The extended coupled-cluster method is formulated as a critical point of an energy function using a generalization of the Rayleigh-Ritz principle: the bivariational principle. This gives a quadratic bound for the energy… Show more

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Cited by 20 publications
(75 citation statements)
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“…This suggests the use of Zarantonello's lemma [48] to characterize local uniqueness and residual bounds. This is in line with previous studies on single-reference CC methods [38,37,21]. We state without proof:…”
Section: Local Uniqueness and Residualsupporting
confidence: 91%
“…This suggests the use of Zarantonello's lemma [48] to characterize local uniqueness and residual bounds. This is in line with previous studies on single-reference CC methods [38,37,21]. We state without proof:…”
Section: Local Uniqueness and Residualsupporting
confidence: 91%
“…For the sake of simplicity we use the same symbols for the Gårding constants ofF as for the Hamiltonian. In complete analogy withĤ, the argument in [15,31] shows that…”
Section: A Gårding Inequality For the Fock Operatormentioning
confidence: 99%
“…In the literature there are two different proofs that the infinite dimensional (continuous) CC function f is locally strongly monotone [17] (see also [31] for the extended CC function). Even though spectral-gap assumptions enter the arguments, it is the so-called Gårding constants that give a sufficient condition for the local strong monotonicity, as will be demonstrated below.…”
Section: B Local Strong Monotonicity Of Thementioning
confidence: 99%
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“…These states are motivated by the analytic solution of the integrable model considered in Section IV, where the excited states with minimal gap have a single quasiparticle excitation. Although mean-field techniques have been highly studied mostly for Hamiltonian systems [48], they can be extended also to non-normal operators [50] where left and right eigenvectors form a bi-orthonormal basis. Within this variational formalism we show in Appendix G that the fourbody interaction in (28) does not alter the eigenstates, which are therefore exactly given by the bare single-particle eigenstates |Ω exc.…”
Section: B Mean-field Approachmentioning
confidence: 99%