Entropy of Isolated Quantum Systems after a Quench

Lea F. Santos, Anatoli Polkovnikov, and Marcos Rigol
Phys. Rev. Lett. 107, 040601 – Published 18 July 2011
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Abstract

A diagonal entropy, which depends only on the diagonal elements of the system’s density matrix in the energy representation, has been recently introduced as the proper definition of thermodynamic entropy in out-of-equilibrium quantum systems. We study this quantity after an interaction quench in lattice hard-core bosons and spinless fermions, and after a local chemical potential quench in a system of hard-core bosons in a superlattice potential. The former systems have a chaotic regime, where the diagonal entropy becomes equivalent to the equilibrium microcanonical entropy, coinciding with the onset of thermalization. The latter system is integrable. We show that its diagonal entropy is additive and different from the entropy of a generalized Gibbs ensemble, which has been introduced to account for the effects of conserved quantities at integrability.

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  • Received 18 January 2011

DOI:https://doi.org/10.1103/PhysRevLett.107.040601

© 2011 American Physical Society

Authors & Affiliations

Lea F. Santos1, Anatoli Polkovnikov2, and Marcos Rigol3,4

  • 1Department of Physics, Yeshiva University, New York, New York 10016, USA
  • 2Department of Physics, Boston University, Boston, Massachusetts 02215, USA
  • 3Department of Physics, Georgetown University, Washington, D.C. 20057, USA
  • 4Kavli Institute for Theoretical Physics, University of California, Santa Barbara, California 93106, USA

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Issue

Vol. 107, Iss. 4 — 22 July 2011

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