Negative stochastic entropy production in quantum trajectories is bounded below by a sharp function of the mean completed entropy, so apparent second-law violations cannot become rarer than a universal floor.
Finite-time bounds on the probabilistic violation of the second law of thermodynamics
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abstract
Jarzynski's equality sets a strong bound on the probability of violating the second law of thermodynamics by extracting work beyond the free energy difference. We derive finite-time refinements to this bound for driven systems in contact with a thermal Markovian environment, which can be expressed in terms of the geometric notion of thermodynamic length. We show that finite-time protocols converge to Jarzynski's bound at a rate slower than $1/\sqrt{\tau}$, where $\tau$ is the total time of the work-extraction protocol. Our result highlights a new application of minimal dissipation processes and demonstrates a connection between thermodynamic geometry and the higher order statistical properties of work.
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Bounds for Apparent Second-Law Violations in Quantum Trajectories
Negative stochastic entropy production in quantum trajectories is bounded below by a sharp function of the mean completed entropy, so apparent second-law violations cannot become rarer than a universal floor.