Experimental observation of a generalized Gibbs ensemble
Detecting multiple temperatures
Most people have an intuitive understanding of temperature. In the context of statistical mechanics, the higher the temperature, the more a system is removed from its lowest energy state. Things become more complicated in a nonequilibrium system governed by quantum mechanics and constrained by several conserved quantities. Langen et al. showed that as many as 10 temperature-like parameters are necessary to describe the steady state of a one-dimensional gas of Rb atoms that was split into two in a particular way (see the Perspective by Spielman).
Abstract
The description of the non-equilibrium dynamics of isolated quantum many-body systems within the framework of statistical mechanics is a fundamental open question. Conventional thermodynamical ensembles fail to describe the large class of systems that exhibit nontrivial conserved quantities, and generalized ensembles have been predicted to maximize entropy in these systems. We show experimentally that a degenerate one-dimensional Bose gas relaxes to a state that can be described by such a generalized ensemble. This is verified through a detailed study of correlation functions up to 10th order. The applicability of the generalized ensemble description for isolated quantum many-body systems points to a natural emergence of classical statistical properties from the microscopic unitary quantum evolution.
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Science
Volume 348 | Issue 6231
10 April 2015
10 April 2015
Copyright
Copyright © 2015, American Association for the Advancement of Science.
Submission history
Received: 5 June 2014
Accepted: 2 March 2015
Published in print: 10 April 2015
Acknowledgments
We acknowledge discussions with E. Demler, E. Dalla Torre, K. Agarwal, J. Berges, M. Karl, V. Kasper, I. Bouchoule, M. Cheneau, and P. Grisins. Supported by the European Union (SIQS and ERC advanced grant QuantumRelax), the Austrian Science Fund (FWF) through the Doctoral Programme CoQuS (W1210) (B.R. and T.S.), the Lise Meitner Programme M1423 (R.G.) and project P22590-N16 (I.E.M.), Deutsche Forschungsgemeinschaft grant GA677/7,8 (T.G.), the University of Heidelberg Center for Quantum Dynamics, Helmholtz Association grant HA216/EMMI, and NSF grant PHY11-25915. T.L., T.G., and J.S. thank the Kavli Institute for Theoretical Physics, Santa Barbara, for its hospitality.
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