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arXiv:1903.08223 · Annales Henri Poincaré

Repeated Interaction Processes in the Continuous-Time Limit, Applied to Quadratic Fermionic Systems

Simon Andréys

Published Sep 30, 2019• 4 citations
arXivHTMLPDF
DOI
10.1007/s00023-019-00852-w

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We consider a model of quantum dynamical semigroup on a finite dimensional fermionic space, obtained as the continuous-time limit of a repeated interactions model between a system and several thermal baths, with a dynamic driven by quadratic Hamiltonians. We assume that there is a globally conserved observable which can be expressed as a sum of energies on the system and on each baths, and we study the energy fluxes between the baths and the system. First, we consider only the mean energy fluxes, and prove that every thermal machines on quasi-free fermions in trivial, in the sense that it is not possible to extract energy from the coolest bath, even when we dispose of several other baths at different temperatures. Then, we consider an unraveling of the semigroup as a random process, and we study the large deviations of the energy fluxes, following Jaksic, Pillet and Westrich (2014). We reduce the computation of the cumulant generating functional to the resolution of a Riccati equation (which is formally similar to the study of large deviations in classical networks of harmonic oscillators). We apply it to the numerical computation of the rate function for energy exchanges in a fermionic chain, and show that larger fluctuations are observed on a longer chain.
We develop an exact framework for quantum Zeno and anti-Zeno dynamics in a broad class of open systems, whose microscopic Hamiltonians are quadratic in bosonic or fermionic operators. We treat the environment through an exact stroboscopic resetting scheme acting at the level of the single-particle density matrix (SPDM). Within this framework, we consider two cases: a repeated-interaction (RI) protocol, in which the environment block is rethermalized and all system-environment coherences are erased after each step, and an evolving-correlation (EC) protocol, in which only the environment block is reset while system-environment coherences are preserved. For RI, we derive a general short-time Zeno law for the survival probability of a single-particle excitation and show that the corresponding decay rate scales linearly with the reset interval, implying Zeno freezing in the limit of infinitely frequent resets. Beyond the short-time regime, we formulate the RI dynamics directly in terms of the exact one-cycle propagator, which allows us to analyze finite-τττ anti-Zeno windows without additional approximations. For EC, we obtain a continuous-reset description in which the kept single-particle correlators obey a finite-dimensional linear differential equation. In this case the drift in the system block remains finite in the frequent-reset limit, so strict freezing is absent. We illustrate these results for a single fermionic level coupled to a semi-infinite tight-binding chain acting as a structured bath. Our results identify coherence erasure versus coherence retention as the key factor controlling the reset-induced Zeno physics.