Exact expectation values within Richardson's approach for the pairing Hamiltonian in a macroscopic system
Gregory Gorohovsky, Eldad Bettelheim

TL;DR
This paper derives exact analytical expectation values for the pairing Hamiltonian in macroscopic systems using Richardson's approach, extending beyond BCS theory to cases with complex excitation spectra.
Contribution
It provides the first analytical expressions for expectation values within Richardson's solution for macroscopic superconductors, generalizing BCS results to more complex spectra.
Findings
Exact expectation values derived for Richardson's pairing Hamiltonian
Results applicable to systems with multiple energy gaps
Generalization of BCS expressions to non-mean-field regimes
Abstract
BCS superconductivity is explained by a simple Hamiltonian describing an attractive pairing interaction between pairs of electrons. The Hamiltonian may be treated using a mean-field method, which is adequate to study equilibrium properties and a variety of nonequilibrium effects. Nevertheless, in certain nonequilibrium situations, even in a macroscopic rather than a microscopic superconductor, the application of mean-field theory may not be valid. In such cases, one may resort to the full solution of the Hamiltonian, as given by Richardson in the 1960s. The relevance of Richardson's solution to macroscopic nonequilibrium superconductors was pointed out recently based on the existence of quantum instabilities out of equilibrium. It is then of interest to obtain analytical expressions for expectation values between exact eigenvalues of the pairing Hamiltonian within the Richardson…
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