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Titlebook: Entropy, Large Deviations, and Statistical Mechanics; Richard S. Ellis Book 1985 Springer-Verlag New York Inc. 1985 Large.Maxwell-Boltzman

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Introduction to Large Deviations theory, which include laws of large numbers and central limit theorems, summarize the behavior of a stochastic system in terms of a few parameters (e.g., mean and variance). In statistical mechanics, one derives macroscopic properties of a substance from a probability distribution that describes th
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Large Deviation Property and Asymptotics of Integralspace. The main results show the exponential decay of large deviation probabilities. A level-1 example is .{|. − .| ≥ .}, where . is the .th partial sum of the random variables and . is their common mean. Levels-2 and 3 treat analogous probabilities for the empirical measures {.} and the empirical pr
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Convex Functions and the Legendre-Fenchel Transforming theme. Suppose that . is a probability measure on ℝ. such that.is finite for all . in ℝ.. The function .(.), called the free energy function of ., is a convex function on ℝ. [Example VII.1.2]. The Legendre-Fenchel transform of .(.) is given by
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Level-2 Large Deviations for I.I.D. Random Vectorsned in Donsker and Varadhan (1975a, 1976a), which prove level-2 large deviation properties for Markov processes taking values in a complete separable metric space.. In Chapter VIII, we will give an elementary, self-contained proof of Theorem I1.4.3 in the special case of i.i.d. random variables with
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Level-3 Large Deviations for I.I.D. Random Vectorsthe special case of i.i.d. random variables with a finite state space. This version of the theorem covers the applications of level-3 large deviations which were made in Chapters III, IV, and V to the Gibbs variational principle. Theorem II.4.4 can also be proved via the methods of Donsker and Varad
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