High-temperature properties of the fcc metallic crystals in anharmonic approximation

J. Tomaszewski, C. Malinowska-Adamska, P. Słoma
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Abstract

The reduced second-order approximation of the self- consistent phonon theory was applied some years ago for cubic metallic crystals those interatomic were approximated by the Morse and Lennard-Jones pair potentials were generally obtained with the help of semi-classical method basin on the classical static relationships between ground- state properties of a crystal and its interatomic potential, and the zero-point vibrations were taken into account only by certain corrections to the experimental data. Moreover, the further self-consistent calculations were being carried out semi-analytically which required some simplifications. In this paper we can reject them because all essential calculations are being carried out numerically. In the studies at high-temperature properties of selected fcc metallic crystal we take as a model of interatomic interactions the Buckingham, Lennard-Jones and Morse pair potentials with the parameters determined self-consistently with the help of the experimental data for the zero-point lattice constant, cohesive energy and isothermal compressibility. Our new theoretical result for pressure variations of the limiting temperatures of dynamical and thermodynamical stability and for the stability criteria are collected and compared with available experimental data.
fcc金属晶体在非谐波近似下的高温特性
自一致声子理论的二阶简化近似是几年前应用于立方金属晶体的,原子间相互作用由莫尔斯和伦纳德-琼斯对势近似,一般借助于半经典方法得到晶体基态性质与其原子间相互作用势之间的经典静态关系。零点振动仅通过对实验数据进行一定的修正来考虑。此外,进一步的自洽计算是半解析的,需要进行一些简化。在本文中,我们可以拒绝它们,因为所有必要的计算都是用数字进行的。在选定的fcc金属晶体的高温性质研究中,我们采用了Buckingham势、Lennard-Jones势和Morse势作为原子间相互作用的模型,这些参数是在零点晶格常数、内聚能和等温压缩率的实验数据的帮助下自一致确定的。本文收集了动力学和热力学稳定极限温度压力变化的新理论结果以及稳定性判据,并与已有的实验数据进行了比较。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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