Abstract
We analyse Landauer’s principle for repeated interaction systems consisting of a reference quantum system \(\mathcal {S}\) in contact with an environment \(\mathcal {E}\) which is a chain of independent quantum probes. The system \(\mathcal {S}\) interacts with each probe sequentially, for a given duration, and Landauer’s principle relates the energy variation of \(\mathcal {E}\) and the decrease of entropy of \(\mathcal {S}\) by the entropy production of the dynamical process. We consider refinements of the Landauer bound at the level of the full statistics (FS) associated with a two-time measurement protocol of, essentially, the energy of \(\mathcal {E}\). The emphasis is put on the adiabatic regime where the environment, consisting of \(T \gg 1\) probes, displays variations of order \(T^{-1}\) between the successive probes, and the measurements take place initially and after T interactions. We prove a large deviation principle and a central limit theorem as \(T \rightarrow \infty \) for the classical random variable describing the entropy production of the process, with respect to the FS measure. In a special case, related to a detailed balance condition, we obtain an explicit limiting distribution of this random variable without rescaling. At the technical level, we obtain a non-unitary adiabatic theorem generalizing that of Hanson et al. (Commun Math Phys 349(1):285–327, 2017) and analyse the spectrum of complex deformations of families of irreducible completely positive trace-preserving maps.
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Communicated by Claude Alain Pillet.
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Hanson, E.P., Joye, A., Pautrat, Y. et al. Landauer’s Principle for Trajectories of Repeated Interaction Systems. Ann. Henri Poincaré 19, 1939–1991 (2018). https://doi.org/10.1007/s00023-018-0679-1
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DOI: https://doi.org/10.1007/s00023-018-0679-1