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The energy of some microscopic stochastic lattices

机译:一些微观随机晶格的能量

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We introduce a notion of energy for some microscopic stochastic lattices. Such lattices are broad generalizations of simple periodic lattices, for which the question of the definition of an energy was examined in a series of previous works [14-18]. Note that slightly more general deterministic geometries were also considered in [6]. These lattices are involved in the modelling of materials whose microscopic structure is a perturbation, in a sense made precise in the article, of the periodic structure of a perfect crystal. The modelling considered here is either a classical modelling, where the sites of the lattice are occupied by ball-like atomic systems that interact by pair potentials, or a quantum modelling where the sites are occupied by nuclei equipped with an electronic structure spread all over the ambient space. The corresponding energies for the infinite stochastic lattices are derived consistently with truncated systems of finite size, by application of a thermodynamic limit process. Subsequent works [7, 8] will be devoted to the macroscopic limits of the energies of such microscopic lattices, thereby extending to a stochastic context the results of [4, 5]. Such convergences in a stochastic setting (in dimension 1) have been studied in [21, 22]. We will also study in [8] some variants and extensions of the stationary setting presented here.
机译:我们引入了一些微观随机晶格的能量概念。这种晶格是简单周期晶格的广义概括,为此,在一系列先前的工作中对能量定义的问题进行了研究[14-18]。注意,在[6]中也考虑了更一般的确定性几何。这些晶格参与了材料的建模,这些材料的微观结构在某种意义上说是对一种完美晶体的周期性结构的扰动,在本文中已作了精确说明。这里考虑的建模要么是经典的建模,即晶格的位置被通过成对电势相互作用的球形原子系统占据,要么是量子建模,其中的位点被配备有遍布整个原子核的电子结构的核占据。环境空间。通过应用热力学极限过程,可以与有限大小的截断系统一致地导出无限随机晶格的相应能量。随后的工作[7,8]将致力于这种微观晶格能量的宏观极限,从而将[4,5]的结果扩展到随机的背景。在[21,22]中已经研究了在随机环境(在维度1)中的这种收敛。我们还将在[8]中研究此处介绍的固定设置的一些变体和扩展。

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