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首页> 外文期刊>Physical Review. B, Condensed Matter >Statistical-thermodynamic description within the ring approximation. Ⅰ. Lattice-gas model
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Statistical-thermodynamic description within the ring approximation. Ⅰ. Lattice-gas model

机译:环近似内的统计热力学描述。 Ⅰ。格子气体模型

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The general method is elaborated for the Statistical-thermodynamic description within the ring approximation of the lattice gas with a complex crystal lattice and with nonpair atomic interactions of any order and effective radii of action. The ring approximation corresponds to the first order of a modified thermodynamic perturbation theory under the choice of the inverse effective number of atoms interacting with one fixed atom as a small parameter of expansion. By the elaborated method one can calculate the complete phase diagram of the lattice gas as well as the correlation effects in both disordered and long-range ordered states of it. The elaborated method is general and analytically simple. The corresponding analytical expressions do not change their form at an increase of the effective radius of atomic interactions and are valid in case of any superstructure. The number of the "variational" parameters for minimization of the free energy is considerably fewer than that within the cluster-variation method and are determined by the type of the superstructure rather than by the value of the effective radius of atomic interactions. Due to the analytical nature of the ring approximation, the time for calculations within it is much less than that of the Monte Carlo simulation. By a comparison with the results of the Monte Carlo simulation the high numerical accuracy of the ring approximation is demonstrated in wide temperature-concentration intervals. The tendency of increase of the numerical accuracy of the ring approximation with increase of the effective radius of atomic interactions is shown. The applicability of the ring approximation is discussed. The obtained results may be useful for a description of solid solutions, alloys, magnetics, fluids, and amorphous materials.
机译:详细阐述了统计热力学描述的一般方法,该方法在具有复杂晶格,具有任意阶数和有效作用半径的不成对原子相互作用的晶格气体的环近似中进行。在选择与一个固定原子相互作用的原子的反有效数量作为小膨胀参数的情况下,环近似对应于改进的热力学微扰理论的一阶。通过精心设计的方法,人们可以计算出晶格气体的完整相图,以及晶格气体在无序和远距离有序状态下的相关效应。精心设计的方法是通用且分析简单。相应的解析表达式不会随着原子相互作用的有效半径的增加而改变其形式,并且在任何上层结构的情况下都是有效的。用于最小化自由能的“可变”参数的数量大大少于簇变量方法中的数量,并且由上层结构的类型而不是由原子相互作用的有效半径的值确定。由于环近似的分析性质,其内的计算时间比蒙特卡洛模拟的时间少得多。通过与蒙特卡洛模拟的结果进行比较,证明了在宽的温度浓度范围内环近似的高数值精度。示出了随着原子相互作用的有效半径的增加,环近似的数值精度增加的趋势。讨论了环近似的适用性。获得的结果对于描述固溶体,合金,磁性,流体和非晶态材料可能有用。

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