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This research investigates whether finite quantum systems can achieve thermodynamic efficiency advantages over classical counterparts by minimizing entropy generation during relaxation processes. The study demonstrates that a few-boson Bose-Hubbard chain retains more microscopic information than its classical field equivalent, leading to higher work output in heat-engine cycles without requiring full state tomography. However, this quantum advantage diminishes as the system scales up toward the classical regime, highlighting the specific operational limits of quantum thermodynamics.
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What this isA model's reading of the article and related coverage, written for aiqbench. Not the publisher's words.

Finite-Particle Quantum Reduction of Thermodynamic Irreversibility

arXiv2 min read

arXiv:2609.10211v1 Announce Type: new Abstract: Thermodynamics is useful because it lets us predict and control complex systems from a few accessible quantities when microscopic reconstruction is impractical. We ask whether this operational reduction can be less costly in a finite quantum system than in a matched classical one. We compare a few-boson Bose--Hubbard chain with its number-conserving classical-field counterpart under the same driving and the same coarse spatial record. The quantum system relaxes more in the observed particle distribution, yet the retained mean energy resolves more of the microscopic structure hidden by that record, leaving less information unusable and smaller entropy generation. We then close the process into a heat-engine cycle whose controls use only the measured mean energy and spatial record, not full state tomography; at matched thermal resources, the smaller entropy generation gives more work and higher efficiency. The advantage fades as the particle number grows toward the classical-field regime.

Abstract:Thermodynamics is useful because it lets us predict and control complex systems from a few accessible quantities when microscopic reconstruction is impractical. We ask whether this operational reduction can be less costly in a finite quantum system than in a matched classical one. We compare a few-boson Bose--Hubbard chain with its number-conserving classical-field counterpart under the same driving and the same coarse spatial record. The quantum system relaxes more in the observed particle distribution, yet the retained mean energy resolves more of the microscopic structure hidden by that record, leaving less information unusable and smaller entropy generation. We then close the process into a heat-engine cycle whose controls use only the measured mean energy and spatial record, not full state tomography; at matched thermal resources, the smaller entropy generation gives more work and higher efficiency. The advantage fades as the particle number grows toward the classical-field regime.

arXiv:2609.10211 [quant-ph]

(or arXiv:2609.10211v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2609.10211 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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Full text under the publisher's open licence · 238 words

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