The coupled-cluster approach to quantum many-body problem in a three-Hilbert-space reinterpretation
arXiv:1311.6295 · doi:10.14311/AP.2014.54.0085
Abstract
The quantum many-body bound-state problem in its computationally successful coupled cluster method (CCM) representation is reconsidered. In conventional practice one factorizes the ground-state wave functions which live in the "physical" Hilbert space using an elementary ansatz for plus a formal expansion of in an operator basis of multi-configurational creation operators. In our paper a reinterpretation of the method is proposed. Using parallels between the CCM and the so called quasi-Hermitian, alias three-Hilbert-space (THS), quantum mechanics, the CCM transition from the known microscopic Hamiltonian (denoted by usual symbol ), which is self-adjoint in , to its effective lower-case isospectral avatar , is assigned a THS interpretation. In the opposite direction, a THS-prescribed, non-CCM, innovative reinstallation of Hermiticity is shown to be possible for the CCM effective Hamiltonian , which only appears manifestly non-Hermitian in its own ("friendly") Hilbert space . This goal is achieved via an ad hoc amendment of the inner product in , thereby yielding the third ("standard") Hilbert space . Due to the resulting exact unitary equivalence between the first and third spaces, , the indistinguishability of predictions calculated in these alternative physical frameworks is guaranteed.
15 pages
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