Area laws and thermalization from classical entropies in a Bose-Einstein condensate

The scaling of local quantum entropies is of utmost interest for characterizing quantum fields, many-body systems, and gravity. Despite their importance, theoretically and experimentally accessing quantum entropies is challenging as they are nonlinear functionals of the underlying quantum state. Her...

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Hauptverfasser: Deller, Yannick (VerfasserIn) , Gärttner, Martin (VerfasserIn) , Haas, Tobias (VerfasserIn) , Oberthaler, Markus K. (VerfasserIn) , Reh, Moritz (VerfasserIn) , Strobel, Helmut (VerfasserIn)
Dokumenttyp: Article (Journal)
Sprache:Englisch
Veröffentlicht: 15 July, 2025
In: Physical review
Year: 2025, Jahrgang: 112, Heft: 1, Pages: 1-7
ISSN:2469-9934
DOI:10.1103/7jzy-g3vd
Online-Zugang:Verlag, lizenzpflichtig, Volltext: https://doi.org/10.1103/7jzy-g3vd
Verlag, lizenzpflichtig, Volltext: https://link.aps.org/doi/10.1103/7jzy-g3vd
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Verfasserangaben:Yannick Deller, Martin Gärttner, Tobias Haas, Markus K. Oberthaler, Moritz Reh, and Helmut Strobel

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520 |a The scaling of local quantum entropies is of utmost interest for characterizing quantum fields, many-body systems, and gravity. Despite their importance, theoretically and experimentally accessing quantum entropies is challenging as they are nonlinear functionals of the underlying quantum state. Here, we show that suitably chosen classical entropies capture many features of their quantum analogs for an experimentally relevant setting. We describe the postquench dynamics of a multiwell spin-1 Bose-Einstein condensate from an initial product state via measurement distributions of spin observables and estimate the corresponding entropies using the asymptotically unbiased -nearest-neighbor method. We observe the dynamical buildup of quantum correlations signaled by an area law, as well as local thermalization revealed by a transition to a volume law, both in regimes characterized by non-Gaussian distributions. We emphasize that all relevant features can be observed at small sample numbers without reconstructing the underlying state or measurement distributions, rendering our method directly applicable to a large variety of models and experimental platforms. 
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