Abstract

We introduce a method to evaluate the steady-state non-equilibrium Keldysh–Schwinger Green’s functions for infinite systems subject to both an electric field and a coupling to reservoirs. The method we present exploits a physical quasi-translation invariance, where a shift by one unit cell leaves the physics invariant if all electronic energies are simultaneously shifted by the magnitude of the electric field. Our framework is straightaway applicable to diagrammatic many-body methods. We discuss two flagship applications, mean-field theories as well as a sophisticated second-order functional renormalization group approach. The latter allows us to push the renormalization-group characterization of phase transitions for lattice fermions into the out-of-equilibrium realm. We exemplify this by studying a model of spinless fermions, which in equilibrium exhibits a Berezinskii–Kosterlitz–Thouless phase transition.

Highlights

  • Unconventional phases of matter play an integral role in condensed matter research and beyond [1]

  • We introduce a method to evaluate the steady-state non-equilibrium Keldysh–Schwinger Green’s functions for infinite systems subject to both an electric field and a coupling to reservoirs

  • The method we present exploits a physical quasi-translation invariance, where a shift by one unit cell leaves the physics invariant if all electronic energies are simultaneously shifted by the magnitude of the electric field

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Summary

14 August 2020

Original content from this work may be used under the terms of the Creative Commons Attribution 4.0 licence. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI. Keywords: strongly correlated electrons, functional renormalization group, non-equilibrium phase transitions

Introduction
Class of models
Green’s functions
Computing Green’s functions in an infinite system
Functional renormalization group approach
Flow equations The flow equation for the self-energy reads
Making use of the system’s symmetry
Retarded single-scale propagator
Keldysh single-scale propagator
Application
Density of states
Phase diagram at intermediate interaction
Conclusion
Full Text
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