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Universal dynamics in an isolated one-dimensional Bose gas far from equilibrium

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TLDR
The results establish universal scaling dynamics in an isolated quantum many-body system, which is a crucial step towards characterizing time evolution far from equilibrium in terms of universality classes.
Abstract
Understanding the behaviour of isolated quantum systems far from equilibrium and their equilibration is one of the most pressing problems in quantum many-body physics1,2. There is strong theoretical evidence that sufficiently far from equilibrium a wide variety of systems—including the early Universe after inflation3–6, quark–gluon matter generated in heavy-ion collisions7–9, and cold quantum gases4,10–14—exhibit universal scaling in time and space during their evolution, independent of their initial state or microscale properties. However, direct experimental evidence is lacking. Here we demonstrate universal scaling in the time-evolving momentum distribution of an isolated, far-from-equilibrium, one-dimensional Bose gas, which emerges from a three-dimensional ultracold Bose gas by means of a strong cooling quench. Within the scaling regime, the time evolution of the system at low momenta is described by a time-independent, universal function and a single scaling exponent. The non-equilibrium scaling describes the transport of an emergent conserved quantity towards low momenta, which eventually leads to the build-up of a quasi-condensate. Our results establish universal scaling dynamics in an isolated quantum many-body system, which is a crucial step towards characterizing time evolution far from equilibrium in terms of universality classes. Universality would open the possibility of using, for example, cold-atom set-ups at the lowest energies to simulate important aspects of the dynamics of currently inaccessible systems at the highest energies, such as those encountered in the inflationary early Universe.

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Quantum Field Theory And Critical Phenomena

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Kinetic Theory of Spin Diffusion and Superdiffusion in XXZ Spin Chains.

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Observation of universal dynamics in a spinor Bose gas far from equilibrium

TL;DR: In this article, the scaling properties of a quantum many-body system were investigated using a spinor Bose-Einstein condensate, and it was shown that the dynamics are governed by an emergent conserved quantity and the transport of spin excitations towards low momentum scales.
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Exploring dynamical phase transitions with cold atoms in an optical cavity

TL;DR: This system uses an ensemble of about a million strontium-88 atoms in an optical cavity to simulate a collective Lipkin–Meshkov–Glick model, an iconic model in quantum magnetism, and reports the observation of distinct dynamical phases of matter in this system.
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Universal prethermal dynamics of Bose gases quenched to unitarity

TL;DR: Degenerate and thermal Bose gases, quenched so that the interparticle interactions are as strong as allowed by quantum mechanics, exhibit dynamics that can be expressed in terms of universal functions.
References
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Journal Article

The Local Structure of Turbulence in Incompressible Viscous Fluid for Very Large Reynolds' Numbers

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Theory of Dynamic Critical Phenomena

TL;DR: The renormalization group theory has been applied to a variety of dynamic critical phenomena, such as the phase separation of a symmetric binary fluid as mentioned in this paper, and it has been shown that it can explain available experimental data at the critical point of pure fluids, and binary mixtures, and at many magnetic phase transitions.
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The renormalization group: Critical phenomena and the Kondo problem

TL;DR: A review of renormalization group ideas in the context of critical phenomena can be found in this paper, where the authors discuss the relationship of the modern renormalisation group to the older problems of divergences in statistical mechanics and field theory.
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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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