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This research advances quantum thermodynamics by refining Jarzynski's equality through the use of coarse-grained endpoint measurements to mitigate sampling inefficiencies in nonequilibrium work trajectories. By defining a maximum-entropy state from accessible macrostates, the study provides an exact statistical control for fluctuation relations within finite Bose-Hubbard systems, significantly reducing computational costs for high-confidence estimates.
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Physical-Work Fluctuation Relations from Accessible Quantum Macrostates

arXiv2 min de cititArticolul și perspectiva sunt în engleză.

arXiv:2610.00246v1 Announce Type: new Abstract: Jarzynski's equality recovers an equilibrium free-energy difference from nonequilibrium work trajectories, but its exponential average can converge very slowly because rare trajectories carry large weight. We show that coarse thermodynamic information measured at the nonequilibrium endpoint can reduce this sampling burden while keeping the same microscopic trajectories and the same free-energy target. The endpoint mean energy and a coarse spatial record define a maximum-entropy state and select one member of an exact family of fluctuation relations. That physically selected member provides an exact statistical control for the ordinary Jarzynski estimator, even when the final energy and retained record do not commute. In a finite Bose--Hubbard system, this control substantially lowers the finite-confidence sampling cost, while a small controlled departure from exact endpoint matching produces a square-root information--sampling tradeoff.

Abstract:Jarzynski's equality recovers an equilibrium free-energy difference from nonequilibrium work trajectories, but its exponential average can converge very slowly because rare trajectories carry large weight. We show that coarse thermodynamic information measured at the nonequilibrium endpoint can reduce this sampling burden while keeping the same microscopic trajectories and the same free-energy target. The endpoint mean energy and a coarse spatial record define a maximum-entropy state and select one member of an exact family of fluctuation relations. That physically selected member provides an exact statistical control for the ordinary Jarzynski estimator, even when the final energy and retained record do not commute. In a finite Bose--Hubbard system, this control substantially lowers the finite-confidence sampling cost, while a small controlled departure from exact endpoint matching produces a square-root information--sampling tradeoff.

Quantum Physics (quant-ph); Statistical Mechanics (cond-mat.stat-mech)

arXiv:2610.00246 [quant-ph]

(or arXiv:2610.00246v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2610.00246 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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