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On the connection between linear combination of entropies and linear combination of extremizing distributions

机译:熵的线性组合与极值分布的线性组合之间的联系

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We analyze the distribution that extremizes a linear combination of the Boltzmann-Gibbs entropy and the nonadditive q-entropy. We show that this distribution can be expressed in terms of a Lambert function. Both the entropic functional and the extremizing distribution can be associated with a nonlinear Fokker-Planck equation obtained from a master equation with nonlinear transition rates. Also, we evaluate the entropy extremized by a linear combination of a Gaussian distribution (which extremizes the Boltzmann-Gibbs entropy) and a q-Gaussian distribution (which extremizes the q-entropy). We give its explicit expression for q = 0, and discuss the other cases numerically. The entropy that we obtain can be expressed, for q = 0, in terms of Lambert functions, and exhibits a discontinuity in the second derivative for all values of q < 1. The entire discussion is closely related to recent results for type-II superconductors and for the statistics of the standard map. (C) 2016 Elsevier B.V. All rights reserved.
机译:我们分析了将Boltzmann-Gibbs熵和非加性q熵的线性组合最大化的分布。我们证明了这种分布可以用Lambert函数表示。熵函数分布和极值分布都可以与从具有非线性跃迁速率的主方程获得的非线性Fokker-Planck方程相关联。同样,我们评估了由高斯分布(对Boltzmann-Gibbs熵进行了极大化)和q-高斯分布(对q熵进行了极大化)的线性组合而得到的熵。我们给出q = 0的显式表达式,并在数值上讨论其他情况。对于q = 0,我们可以用Lambert函数表示熵,并且对于所有q <1的值,其二阶导数都具有不连续性。整个讨论与II型超导体的最新结果密切相关。以及用于标准地图的统计信息。 (C)2016 Elsevier B.V.保留所有权利。

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