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Complete Generalized Gibbs Ensembles in an Interacting Theory

Enej IlievskiInstitute for Theoretical Physics, University of Amsterdam, Science Park 904, 1098 XH Amsterdam, The NetherlandsJacopo De NardisInstitute for Theoretical Physics, University of Amsterdam, Science Park 904, 1098 XH Amsterdam, The NetherlandsB. WoutersInstitute for Theoretical Physics, University of Amsterdam, Science Park 904, 1098 XH Amsterdam, The NetherlandsJean-Sébastien CauxInstitute for Theoretical Physics, University of Amsterdam, Science Park 904, 1098 XH Amsterdam, The NetherlandsFabian H. L. EßlerThe Rudolf Peierls Centre for Theoretical Physics, University of Oxford, Oxford OX1 3NP, United KingdomTomaž ProsenFaculty of Mathematics and Physics, University of Ljubljana, Jadranska 19, SI-1000 Ljubljana, Slovenia
2015en
ABI

Аннотация

In integrable many-particle systems, it is widely believed that the stationary state reached at late times after a quantum quench can be described by a generalized Gibbs ensemble (GGE) constructed from their extensive number of conserved charges. A crucial issue is then to identify a complete set of these charges, enabling the GGE to provide exact steady-state predictions. Here we solve this long-standing problem for the case of the spin-1/2 Heisenberg chain by explicitly constructing a GGE which uniquely fixes the macrostate describing the stationary behavior after a general quantum quench. A crucial ingredient in our method, which readily generalizes to other integrable models, are recently discovered quasilocal charges. As a test, we reproduce the exact postquench steady state of the Néel quench problem obtained previously by means of the Quench Action method.

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