Abstract

This article presents an overview on recent progress in the theory of nonequilibrium Green functions (NEGF). We discuss applications of NEGF simulations to describe the femtosecond dynamics of various finite fermionic systems following an excitation out of equilibrium. This includes the expansion dynamics of ultracold atoms in optical lattices following a confinement quench and the excitation of strongly correlated electrons in a solid by the impact of a charged particle. NEGF, presently, are the only ab initio quantum approach that is able to study the dynamics of correlations for long times in two and three dimensions. However, until recently, NEGF simulations have mostly been performed with rather simple selfenergy approximations such as the second-order Born approximation (SOA). While they correctly capture the qualitative trends of the relaxation towards equilibrium, the reliability and accuracy of these NEGF simulations has remained open, for a long time.Here we report on recent tests of NEGF simulations for finite lattice systems against exact-diagonalization and density-matrix-renormalization-group benchmark data. The results confirm the high accuracy and predictive capability of NEGF simulations—provided selfenergies are used that go beyond the SOA and adequately include strong correlation and dynamical-screening effects. With an extended arsenal of selfenergies that can be used effectively, the NEGF approach has the potential of becoming a powerful simulation tool with broad areas of new applications including strongly correlated solids and ultracold atoms. The present review aims at making such applications possible. To this end we present a selfcontained introduction to the theory of NEGF and give an overview on recent numerical applications to compute the ultrafast relaxation dynamics of correlated fermions. In the second part we give a detailed introduction to selfenergies beyond the SOA. Important examples are the third-order approximation, the approximation, the T-matrix approximation and the fluctuating-exchange approximation. We give a comprehensive summary of the explicit selfenergy expressions for a variety of systems of practical relevance, starting from the most general expressions (general basis) and the Feynman diagrams, and including also the important cases of diagonal basis sets, the Hubbard model and the differences occuring for bosons and fermions. With these details, and information on the computational effort and scaling with the basis size and propagation duration, readers will be able to choose the proper basis set and straightforwardly implement and apply advanced selfenergy approximations to a broad class of systems.

Highlights

  • This article presents an overview on recent progress in the theory of nonequilibrium Green functions (NEGF)

  • The results confirm the high accuracy and predictive capability of NEGF simulations—provided selfenergies are used that go beyond the second-order approximation (SOA) and adequately include strong correlation and dynamical-screening effects

  • For approach I.) that starts with the bare interaction, Eq (97), we will consider:

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Summary

Summary of selfenergy approximations

We list the selfenergies that will be discussed in this paper and briefly summarize their respective strengths and weaknesses. Spectral function generated from different selfenergy approximations: brown full line: third-order approximation (TOA), crimson dashed line: second-order approximation (SOA), green dashed line: particle–particle T matrix (TPP), yellow dashed line: electron– hole T matrix (TEH), blue dashed line: GW approximation (GWA), purple semi-dashed line: fluctuating-exchange approximation (FLEX), gray full line: Hartree–Fock approximation (HF). Summarizing the ability of NEGF methods to describe the spectral function of Hubbard clusters, one can state that the overall agreement for small to medium interaction strength is good and especially via combination of different approximation methods as well as probing from both systems with adjacent number of particles, one can gain a large part of the spectral information

Time evolution following an external excitation
Second-order selfenergy contributions
Third-order term
Second-order vertex terms
Third-order terms
Resummation approaches
Resummation approaches: T matrix
General basis
Diagonal basis
Hubbard basis
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