Lehmann representation of the nonequilibrium self-energy
Christian Gramsch, Michael Potthoff

TL;DR
This paper establishes a unique Lehmann representation for the non-equilibrium self-energy of lattice fermion models and introduces a numerically efficient scheme to compute it, enabling longer time simulations and better understanding of non-equilibrium dynamics.
Contribution
It provides a novel Lehmann representation for the non-equilibrium self-energy and an explicit, practical scheme to construct it from Green's functions, improving long-time numerical simulations.
Findings
Efficient scheme extends maximum propagation time in Dyson's equation solutions.
Demonstrates applicability to Hubbard model quench dynamics on a 10x10 lattice.
Shows moderate violation of conservation laws and captures prethermalization phenomena.
Abstract
It is shown that the non-equilibrium self-energy of an interacting lattice-fermion model has a unique Lehmann representation. Based on the construction of a suitable non-interacting effective medium, we provide an explicit and numerically practicable scheme to construct the Lehmann representation for the self-energy, given the Lehmann representation of the single-particle non-equilibrium Green's function. This is of particular importance for an efficient numerical solution of Dyson's equation in the context of approximations where the self-energy is obtained from a reference system with a small Hilbert space. As compared to conventional techniques to solve Dyson's equation on the Keldysh contour, the effective-medium approach allows to reach a maximum propagation time which can be several orders of magnitude longer. This is demonstrated explicitly by choosing the non-equilibrium…
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