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Quantum many-body thermal machines enabled by atom-atom correlations

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arxiv 2308.05266 v5 pith:4JZSJ4TJ submitted 2023-08-10 cond-mat.quant-gas cond-mat.stat-mechquant-ph

classification cond-mat.quant-gascond-mat.stat-mechquant-ph
keywords quantumcorrelationsthermalatom-atommachinesmany-bodyenabledphysics
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Particle-particle correlations, characterized by Glauber's second-order correlation function,play an important role in the understanding of various phenomena in radio and optical astronomy, quantum and atom optics, particle physics, condensed matter physics, and quantum many-body theory. However, the relevance of such correlations to quantum thermodynamics has so far remained illusive. Here, we propose and investigate a class of quantum many-body thermal machines whose operation is directly enabled by second-order atom-atom correlations in an ultracold atomic gas. More specifically, we study quantum thermal machines that operate in a sudden interaction-quench Otto cycle and utilize a one-dimensional Lieb-Liniger gas of repulsively interacting bosons as the working fluid. The atom-atom correlations in such a gas are different to those of a classical ideal gas, and are a result of the interplay between interparticle interactions, quantum statistics, and thermal fluctuations. We show that operating these thermal machines in the intended regimes, such as a heat engine, refrigerator, thermal accelerator, or heater, would be impossible without such atom-atom correlations. Our results constitute a step forward in the design of conceptually new quantum thermodynamic devices which take advantage of uniquely quantum resources such as quantum coherence, correlations, and entanglement.

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  1. Emergence of thermodynamic functioning regimes from finite coupling between a quantum thermal machine and a load

    quant-ph 2025-06 conditional novelty 6.0 of 10

    Finite machine-load coupling turns a simple three-level thermal machine into a four-regime device where stronger coupling suppresses engine and refrigerator operation and the load's initial occupation acts as a control knob.

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