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A quantum Newton's cradle

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TLDR
In this paper, the authors show that a homogeneous 1D Bose gas with point-like collisional interactions is integrable, and that it is possible to construct a system with many degrees of freedom that does not reach thermal equilibrium even after thousands of collisions.
Abstract
It is a fundamental assumption of statistical mechanics that a closed system with many degrees of freedom ergodically samples all equal energy points in phase space. To understand the limits of this assumption, it is important to find and study systems that are not ergodic, and thus do not reach thermal equilibrium. A few complex systems have been proposed that are expected not to thermalize because their dynamics are integrable. Some nearly integrable systems of many particles have been studied numerically, and shown not to ergodically sample phase space. However, there has been no experimental demonstration of such a system with many degrees of freedom that does not approach thermal equilibrium. Here we report the preparation of out-of-equilibrium arrays of trapped one-dimensional (1D) Bose gases, each containing from 40 to 250 87Rb atoms, which do not noticeably equilibrate even after thousands of collisions. Our results are probably explainable by the well-known fact that a homogeneous 1D Bose gas with point-like collisional interactions is integrable. Until now, however, the time evolution of out-of-equilibrium 1D Bose gases has been a theoretically unsettled issue, as practical factors such as harmonic trapping and imperfectly point-like interactions may compromise integrability. The absence of damping in 1D Bose gases may lead to potential applications in force sensing and atom interferometry.

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Many-Body Physics with Ultracold Gases

TL;DR: In this article, a review of recent experimental and theoretical progress concerning many-body phenomena in dilute, ultracold gases is presented, focusing on effects beyond standard weakcoupling descriptions, such as the Mott-Hubbard transition in optical lattices, strongly interacting gases in one and two dimensions, or lowest-Landau-level physics in quasi-two-dimensional gases in fast rotation.
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Thermalization and its mechanism for generic isolated quantum systems

TL;DR: It is demonstrated that a generic isolated quantum many-body system does relax to a state well described by the standard statistical-mechanical prescription, and it is shown that time evolution itself plays a merely auxiliary role in relaxation, and that thermalization instead happens at the level of individual eigenstates, as first proposed by Deutsch and Srednicki.
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Colloquium: Nonequilibrium dynamics of closed interacting quantum systems

TL;DR: In this paper, the authors give an overview of recent theoretical and experimental progress in the area of nonequilibrium dynamics of isolated quantum systems, particularly focusing on quantum quenches: the temporal evolution following a sudden or slow change of the coupling constants of the system Hamiltonian.
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Observation of many-body localization of interacting fermions in a quasirandom optical lattice

TL;DR: This experiment experimentally observed this nonergodic evolution for interacting fermions in a one-dimensional quasirandom optical lattice and identified the MBL transition through the relaxation dynamics of an initially prepared charge density wave.
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Quantum many-body systems out of equilibrium

TL;DR: In this article, the authors provide an overview of the progress in probing dynamical equilibration and thermalization of closed quantum many-body systems driven out of equilibrium by quenches, ramps and periodic driving.
References
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Journal ArticleDOI

Ultracold atoms and the Functional Renormalization Group

TL;DR: In this paper, a self-contained introduction to the physics of ultracold atoms using functional integral techniques is given, and the universal effective low energy Hamiltonian is derived based on a consideration of the relevant length scales.
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Observation of a persistent non-equilibrium state in cold atoms

TL;DR: In this paper, the authors report a long-delayed vindication for Boltzmann: the observation of a 3D monopole mode for which the collisional contribution to damping vanishes.
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Dynamic finite-size scaling after a quench at quantum transitions.

TL;DR: A general dynamic finite-size scaling theory for the quantum dynamics after an abrupt quench is presented, at both continuous and first-order quantum transitions, and the dynamic scaling laws are supported by numerical evidence.
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Fermionisation dynamics of a strongly interacting 1D Bose gas after an interaction quench

TL;DR: In this paper, the authors studied the dynamics of a Bose gas after a sudden change of the interaction strength from zero to a finite value using the numerical time-evolving block decimation (TEBD) algorithm.
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Probing Ground-State Phase Transitions through Quench Dynamics

TL;DR: In this article, the authors show that the fundamental ingredients of quantum phase transitions can be probed directly with quench dynamics in integrable and nearly-integrable systems.