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Quantum moment hydrodynamics and the entropy principle

机译:量子矩流体力学和熵原理

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This paper presents how a non-commutative version of the entropy extremalization principle allows to construct new quantum hydrodynamic models. Our starting point is the moment method, which consists in integrating the quantum Liouville equation with respect to momentum p against a given vector of monomials of p. Like in the classical case, the so-obtained moment system is not closed. Inspired from Levermore's procedure in the classical case,((26)) we propose to close the moment system by a quantum (Wigner) distribution function which minimizes the entropy subject to the constraint that its moments are given. In contrast to the classical case, the quantum entropy is defined globally ( and not locally) as the trace of an operator. Therefore, the relation between the moments and the Lagrange multipliers of the constrained entropy minimization problem becomes nonlocal and the resulting moment system involves nonlocal operators (instead of purely local ones in the classical case). In the present paper, we discuss some practical aspects and consequences of this nonlocal feature. [References: 37]
机译:本文介绍了熵极值化原理的非交换形式如何允许构造新的量子流体动力学模型。我们的出发点是矩量法,该方法包括将p动量p的量子Liouville方程与p的单项式的给定向量进行积分。像经典情况一样,如此获得的力矩系统也不是封闭的。受经典案例中Levermore程序的启发,((26)),我们建议通过量子(Wigner)分布函数来封闭矩系统,该函数在给定矩的约束下使熵最小。与经典情况相反,量子熵被全局(而不是局部地)定义为算符的轨迹。因此,约束熵最小化问题的矩与拉格朗日乘数之间的关系变为非局部,并且所得的矩系统包含非局部算子(而不是经典情况下的纯局部算子)。在本文中,我们讨论了此非本地功能的一些实际方面和后果。 [参考:37]

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