Decay and recurrence of non-Gaussian correlations in a quantum many-body
system
- URL: http://arxiv.org/abs/2003.01808v2
- Date: Thu, 2 Sep 2021 05:00:35 GMT
- Title: Decay and recurrence of non-Gaussian correlations in a quantum many-body
system
- Authors: Thomas Schweigler, Marek Gluza, Mohammadamin Tajik, Spyros Sotiriadis,
Federica Cataldini, Si-Cong Ji, Frederik S. M{\o}ller, Jo\~ao Sabino,
Bernhard Rauer, Jens Eisert, and J\"org Schmiedmayer
- Abstract summary: We observe a non-Gaussian initial state evolving under non-interacting dynamics in a quantum many-body system.
This non-equilibrium evolution is triggered by abruptly switching off the effective interaction between the observed collective degrees of freedom.
A description of this dynamics requires a novel mechanism for the emergence of Gaussian correlations.
- Score: 0.45823749779393547
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: Gaussian models provide an excellent effective description of many quantum
many-body systems ranging from condensed matter systems all the way to neutron
stars. Gaussian states are common at equilibrium when the interactions are
weak. Recently it was proposed that they can also emerge dynamically from a
non-Gaussian initial state evolving under non-interacting dynamics. In this
work, we present the experimental observation of such a dynamical emergence of
Gaussian correlations in a quantum many-body system. This non-equilibrium
evolution is triggered by abruptly switching off the effective interaction
between the observed collective degrees of freedom, while leaving the
interactions between the microscopic constituents unchanged. Starting from
highly non-Gaussian correlations, consistent with the sine-Gordon model, we
observe a Gaussian state to emerge over time as revealed by the decay of the
fourth and sixth order connected correlations in the quantum field. A
description of this dynamics requires a novel mechanism for the emergence of
Gaussian correlations, which is relevant for a wide class of quantum many-body
systems. In our closed system with non-interacting effective degrees of
freedom, we do not expect full thermalization. This memory of the initial state
is confirmed by observing recurrences of non-Gaussian correlations.
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