2022
DOI: 10.48550/arxiv.2204.08059
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Large deviations for quadratic functionals of stable Gauss-Markov chains and entropy production

Abstract: In this paper we establish a large deviation principle for the entropy production rate of possible non-stationary, centered stable Gauss-Markov chains, verifying the Gallavotti-Cohen symmetry. We reach this goal by developing a large deviation theory for quasi-Toeplitz quadratic functionals of multivariate centered stable Gauss-Markov chains, which differ from a perfect Toeplitz form by the addition of quadratic boundary terms.

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Cited by 2 publications
(2 citation statements)
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“…A large deviation theory beyond Poissonian resetting allows to appreciate the emergence of singularities in the graph of their rate functions, which are interpreted as dynamical phase transitions. Dynamical phase transitions have been already documented for time-averaged quantities such as the heat exchanged after a quench [27,28], the heat exchanged between two thermal walls [29,30], the active work in active matter [31], the total displacement of random walks [32][33][34][35], occupation times of a Brownian particle [36,37], and the entropy production [38][39][40][41][42]. Physicists often invoke the Gärtner-Ellis theorem to justify their calculations that lead to dynamical phase transitions, although it is necessary for a dynamical phase transition to occur that the hypotheses of that theorem are violated.…”
Section: Introductionmentioning
confidence: 99%
“…A large deviation theory beyond Poissonian resetting allows to appreciate the emergence of singularities in the graph of their rate functions, which are interpreted as dynamical phase transitions. Dynamical phase transitions have been already documented for time-averaged quantities such as the heat exchanged after a quench [27,28], the heat exchanged between two thermal walls [29,30], the active work in active matter [31], the total displacement of random walks [32][33][34][35], occupation times of a Brownian particle [36,37], and the entropy production [38][39][40][41][42]. Physicists often invoke the Gärtner-Ellis theorem to justify their calculations that lead to dynamical phase transitions, although it is necessary for a dynamical phase transition to occur that the hypotheses of that theorem are violated.…”
Section: Introductionmentioning
confidence: 99%
“…A large deviation theory beyond Poissonian resetting allows us to appreciate the emergence of singularities in the graph of their rate functions, which are interpreted as dynamical phase transitions. Dynamical phase transitions have been already documented for time-averaged quantities such as the heat exchanged after a quench [37,38], the active work in active matter [39], the total displacement of random walks [40][41][42][43], occupation times of a Brownian particle [44,45], and the entropy production [46][47][48][49][50]. Physicists often invoke the Gärtner-Ellis theorem to justify their calculations that lead to dynamical phase transitions, although it is necessary for a dynamical phase transition to occur that the hypotheses of that theorem are violated.…”
Section: Introductionmentioning
confidence: 99%