II-IV-V2和I-III-VI2中红外非线性光学晶体:肖特基缺陷浓度

V. Voevodin, O. Voevodina
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引用次数: 3

摘要

本文研究了I- III-VI2型和ii - iv - v2型三元非线性光学晶体。采用准化学反应的理论热力学方法。空位熵计算为构型分量和振动分量之和。对于第一种方法,当一个一致原子被删除时,未配对电子形成的新键位置的不确定性产生,并且考虑了弛豫原子新位置的不确定性。采用了构型熵(Delta) Sconf = (Sigma)的标准玻尔兹曼表达式和几何考虑。假设振动分量是由形成空位周围原子振动频率的变化引起的。考虑了键长和成键力的变化。振动熵变(Delta)的近似表达式Svibr = 3Nkln,采用几何考虑和键长计算结果。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
II-IV-V2 and I-III-VI2 nonlinear optical crystals for mid-IR range: Schottky defects concentration
The work deals with ternary nonlinear optical crystals of I- III-VI2, and II-IV-V2-type. Theoretical thermodynamic method of quasi-chemical reactions was used. Entropy of vacancy was calculated as sum of configuration and vibration components. For the first one uncertainty in positions of new bonds formed by unpaired electrons arisen when one of consistent atoms is deleted and uncertainty in new positions of relaxing atoms were considered. Standard Boltzmann expression for configuration entropy (Delta) Sconf equals (Sigma) klnw and geometry considerations were used. It was assumed that the vibration component is caused by change in vibration frequency of atoms surrounding formed vacancy. Change in length of bonds and in bonding force took into account. Approximate expression for vibration entropy change (Delta) Svibr equals 3Nkln, geometry considerations and results of bonds lengths calculations were used.
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