Equilibration and GGE in interacting-to-free Quantum Quenches in dimensions d>1
Spyros Sotiriadis, Gabriele Martelloni

TL;DR
This paper demonstrates that in higher-dimensional quantum field theories, long-time evolution under free dynamics causes initial interacting ground states to effectively become Gaussian, with local observables described by a generalized Gibbs ensemble, extending previous 1D results.
Contribution
It generalizes the known 1D GGE results to higher dimensions, showing that interacting ground states evolve towards a Gaussian state characterized by initial two-point correlations.
Findings
Connected correlation functions decay over time.
Local observables equilibrate to Gaussian values.
GGE accurately describes asymptotic correlation behaviour.
Abstract
Ground states of interacting QFTs are non-gaussian states, i.e. their connected n-point correlation functions do not vanish for n>2, in contrast to the free QFT case. We show that when the ground state of an interacting QFT evolves under a free massive QFT for a long time (a scenario that can be realised by a Quantum Quench), the connected correlation functions decay and all local physical observables equilibrate to values that are given by a gaussian density matrix that keeps memory only of the two-point initial correlation function. The argument hinges upon the fundamental physical principle of cluster decomposition, which is valid for the ground state of a general QFT. An analogous result was already known to be valid in the case of d=1 spatial dimensions, where it is a special case of the so-called Generalised Gibbs Ensemble (GGE) hypothesis, and we now generalise it to higher…
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