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Noncommutative pressure and the variational principle in Cuntz-Krieger-type C*-algebras

机译:Cuntz-Krieger型C *-代数的非交换压力和变分原理

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Let a be a self-adjoint element of an exact C*-algebra A and theta: A --> A a contractive completely positive map. We define a notion of dynamical pressure Petal which adopts Voiculescu's approximation approach to noncommutative entropy and extends the Voiculescu-Brown topological entropy and Neshveyev and Stormer unital-nuclear pressure. A variational inequality bounding P (a) below by the free energies h(sigma)(theta) + sigma(a) with respect to the Sauvageot Thouvenot entropy h(sigma)(theta) is established in two stages via the introduction of a local state approximation entropy, whose associated free energies function as an intermediate term. Pimsner C*-algebras furnish a framework for investigating the variational principle, which asserts the equality of P-theta(a) with the supremum of the free energies over all theta-invariant states. In one direction we extend Brown's result on the constancy of the Voiculescu Brown entropy upon passing to the crossed product, and in another we show that the pressure of a self-adjoint element over the Markov subshift underlying the canonical map on the Cuntz-Krieger algebra O-A is equal to its classical pressure. The latter result is extended to a more general setting comprising an expanded class of Cuntz Krieger-type Pimsner algebras, leading to the variational principle for self-adjoint elements in a diagonal subalgebra. Equilibrium states are constructed from KMS states under certain conditions in the case of Cuntz Krieger algebras. (C) 2002 Elsevier Science (USA). [References: 33]
机译:令a为精确C *代数A和theta的自伴元素:A-> A收缩的完全正图。我们定义了动态压力瓣的概念,该瓣采用Voiculescu的逼近方法进行非交换熵,并扩展了Voiculescu-Brown拓扑熵以及Neshveyev和Stormer单位核压力。通过引入局部方程,在两个阶段建立了相对于Sauvageot Thouvenot熵h(sigma)(theta)的以自由能h(sigma)(theta)+ sigma(a)为边界的变分不等式P(a)状态近似熵,其相关的自由能用作中间项。 Pimsner C *-代数提供了一个研究变分原理的框架,该论断断言P-theta(a)与所有theta不变态的自由能至上相等。在一个方向上,我们将布朗的结果扩展到Voiculescu布朗熵在传递给叉积时的恒定性,而在另一个方向上,我们证明了Cuntz-Krieger代数正则图基础上马尔可夫子移位上自伴元素的压力OA等于其经典压力。后者的结果扩展到一个更通用的设置,其中包括Cuntz Krieger型Pimsner代数的扩展类,从而得出对角子代数中自伴元素的变分原理。对于Cuntz Krieger代数,在某些条件下根据KMS状态构造平衡状态。 (C)2002 Elsevier Science(美国)。 [参考:33]

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