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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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Citations
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Thermalization of Bipartite Bose-Hubbard Models.

TL;DR: The time evolution of a bipartite Bose-Hubbard model prepared far from equilibrium is studied to observe ergodization of the number distribution and a constant increase of the entanglement entropy between the constituent subsystems until it saturates to thermal equilibrium values.
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Relaxation of Bosons in One Dimension and the Onset of Dimensional Crossover

TL;DR: In this article, the authors study ultra-cold bosons out of equilibrium in a 1D setting and probe the breaking of integrability and the resulting relaxation at the onset of the crossover from one to three dimensions.
Journal ArticleDOI

Thermalization in Systems with Bipartite Eigenmode Entanglement

TL;DR: In this paper, it was shown that the asymptotic correlations in exactly solvable models following a quantum quench can behave essentially as thermal correlations provided the entanglement between two eigenmodes is sufficiently strong.
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Form factors in equilibrium and non-equilibrium mixed states of the Ising model

TL;DR: In this paper, the authors studied the case of mixed states that are diagonal in the asymptotic particle basis, and obtained exact expressions for all mixed-state form factors of order and disorder fields.
Dissertation

Out-Of-Equilibrium Dynamics and Locality in Long-Range Many-Body Quantum Systems

TL;DR: In this article, the propagation of correlations in long-range interacting quantum systems has been studied and analytical expressions to describe the time evolution of generic observables in systems where the Hamiltonian takes a quadratic form with long-and short-range interactions.
References
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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.
Journal ArticleDOI

Exact analysis of an interacting bose gas. i. the general solution and the ground state

TL;DR: In this paper, the ground-state energy as a function of γ was derived for all γ, except γ = 0, and it was shown that Bogoliubov's perturbation theory is valid when γ is small.
Journal ArticleDOI

From quantum chaos and eigenstate thermalization to statistical mechanics and thermodynamics

TL;DR: The eigenstate thermalization hypothesis (ETH) as discussed by the authors is a natural extension of quantum chaos and random matrix theory (RMT) that allows one to describe thermalization in isolated chaotic systems without invoking the notion of an external bath.