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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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Nonadiabatic dynamics of a dissipative spin chain in a transverse magnetic field

TL;DR: In this article, a non-Hermitian Hamiltonian is proposed to describe a dissipative spin chain in a transverse magnetic field, and the time evolution of the transition probabilities is formulated and derived in terms of the normalized density operator of the model.
Dissertation

Quebra da integrabilidade para um modelo de tunelamento quântico de três poços

TL;DR: In this paper, an integrable model that describes the tunneling of bosons between three coupled aligned Bose-Einstein condensates is presented and investigated, where the integrability means that the model can be exactly solved by the Bethe Ansatz method.
Journal ArticleDOI

Faddeev equations in one-dimensional problems with resonant interactions

TL;DR: In this paper, the problem of three one-dimensional bosons with resonant multichannel interactions was reduced to a single-channel Faddeev-Lovelace equation by elimination of the closed and output channels.
Journal ArticleDOI

Particle injection into a chain: decoherence versus relaxation for Hermitian and non‐Hermitian dynamics

TL;DR: In this article, a model for the injection of fermionic particles from filled source sites into an empty chain is investigated, and the ensuing dynamics for Hermitian as well as for non-Hermitian time evolution, where the particles cannot return to the bath sites (quantum ratchet), is studied.
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Dynamics of the Bose-Hubbard chain for weak interactions

TL;DR: In this article, the Boltzmann transport equation for the Bose-Hubbard chain in the kinetic regime was studied and the authors provided a derivation based on the Hubbard Hamiltonian, including general interactions beyond on-site.
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.