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Real-time confinement following a quantum quench to a non-integrable model

TLDR
In this paper, the authors show that confinement has dramatic consequences for the non-equilibrium dynamics following a quantum quench and that these effects could be exploited as a quantitative probe of confinement.
Abstract
Confinement plays an important role in many-body physics from high energy to condensed matter. New results show that it strongly affects the non-equilibrium dynamics after a quantum quench with possible implications from ultracold atoms to QCD. Quarks cannot be observed as free particles in nature because they are confined into baryons and mesons, as a result of the fact that the strong interaction between them increases with their separation. However, it is less known that this phenomenon also occurs in condensed matter and statistical physics as experimentally proved in several quasi-1D compounds1,2. Most of the theoretical and experimental studies so far concentrated on understanding the consequences of confinement for the equilibrium physics of both high-energy and condensed matter systems. Here, instead we show that confinement has dramatic consequences for the non-equilibrium dynamics following a quantum quench and that these effects could be exploited as a quantitative probe of confinement.

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A quantum Newton's cradle

TL;DR: 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.
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Entanglement and thermodynamics after a quantum quench in integrable systems

TL;DR: It is shown that the standard quasiparticle picture of the entanglement evolution, complemented with integrability-based knowledge of the steady state and its excitations, leads to a complete understanding of theEntanglement dynamics in the space–time scaling limit.
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Quantum Many-Body Scars and Weak Breaking of Ergodicity

TL;DR: In this article, the authors provide a pedagogical introduction to quantum many-body scars and highlight the newly emerged connections with the semiclassical quantization of many body systems, and discuss the relation between scars and more general routes towards weak violations of ergodicity due to embedded algebras and non-thermal eigenstates.
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Exact Quantum Many-Body Scar States in the Rydberg-Blockaded Atom Chain.

TL;DR: It is shown that the nearby many-body scar states can be well approximated as "quasiparticle excitations" on top of the exact E=0 scar states and proposed a quasiparticles explanation of the strong oscillations observed in experiments.
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Simulating quantum many-body dynamics on a current digital quantum computer

TL;DR: In this article, state-of-the-art IBM quantum computers are used to simulate the effects of disorder and interactions on quantum particle transport, as well as correlation and entanglement spreading.
References
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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.
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A quantum Newton's cradle

TL;DR: The preparation of out-of-equilibrium arrays of trapped one-dimensional Bose gases, each containing from 40 to 250 87Rb atoms, which do not noticeably equilibrate even after thousands of collisions are reported.
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The Finite Group Velocity of Quantum Spin Systems

TL;DR: In this paper, it was shown that information can propagate in a quantum spin system only with a finite group velocity, where μ(ν) > 0, where ρ is the group velocity.
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Evolution of entanglement entropy in one-dimensional systems

TL;DR: In this paper, the authors studied the unitary time evolution of the entropy of entanglement of a one-dimensional system between the degrees of freedom in an interval of length and its complement, starting from a pure state which is not an eigenstate of the Hamiltonian.
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Time-dependence of correlation functions following a quantum quench

TL;DR: It is shown that the time dependence of correlation functions in an extended quantum system in d dimensions, which is prepared in the ground state of some Hamiltonian and then evolves without dissipation according to some other Hamiltonian, may be extracted using methods of boundary critical phenomena in d + 1 dimensions.
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