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Work extractability from energy eigenstates under optimized local operations
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We examine the relationship between the second law of thermodynamics and the energy eigenstates of quantum many-body systems that undergo cyclic unitary evolution. Using a numerically optimized control protocol, we analyze how the work extractability is affected by the integrability of the system. Our findings reveal that, in nonintegrable systems the number of work-extractable energy eigenstates converges to zero, even when the local control operations are optimized. In contrast, in integrable systems, there are exponentially many eigenstates from which positive work can be extracted, regardless of the locality of the control operations. We numerically demonstrate that such a strikingly different behavior can be attributed to the number of athermal energy eigenstates. Our results provide insights into the foundations of the second law of thermodynamics in isolated quantum many-body systems, which are expected to contribute to the development of quantum many-body heat engines.
Forward citations
Cited by 2 Pith papers
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Second law of thermodynamics in closed quantum many-body systems
Pure quantum states that are macroscopically equivalent to a Gibbs state for every additive observable obey Planck's principle and a law of increasing entropy under macroscopic operations of size-independent duration.
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Typical Positivity of Nonequilibrium Entropy Production for Pure States
For almost all pure states sampled from the Scrooge measure, entropy production is exponentially close to the ensemble value, so typical pure states obey the second law.
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