Phase equilibria in Cd0.80Mn0.20Te solid solutions

A. V. Matviy, V. V. Kopach, S. M. Rusnak, O. Kopach, L. Shcherbak, P. Fochuk
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Abstract

The thermal properties of Cd0.80Mn0.20Te solid solutions were investigated in this article. Two methods of heat treatment were used for thermography of alloys, which allowed investigating their thermal properties. One of the methods of thermography of samples was to heat them to the maximum temperature at which they were kept for a certain time, followed by cooling of the sample. The data obtained by this type of thermography allow obtaining graphs which characterized the crystallization parameters of the melt Cd0.80Mn0.20Te. It is shown that the crystallization of the Cd0.80Mn0.20Te melt occurs without supercooling at its overheating less than 14 °С in comparison with the beginning of melting temperature, which indicates the two-phase melt. It is also shown that the crystallization rate of the Cd0.80Mn0.20Te melt increases with decreasing crystallization temperature. Thermography of alloys by the second method of heat treatment is to conduct a series of isothermal holding during heating of the samples to the maximum temperature (1150 °C). Thus, the parameters of alloy melting were investigated. It was determined that the volume fraction of solid phase in the Cd0.80Mn0.20Te melt decreases from 100% to 0% in the temperature range 1078-1095 °С. Based on the obtained data of differential thermal analyses the Cd0.80Mn0.20Te ingot was grown under controlled conditions. After cutting this crystal we can see several monocrystalline areas of different sizes. IR microscope showed that the minimum number of inclusions <7 mm in diameter distributed in different parts of the sample The value of the band gap in all samples ranges from 1.78 to 1.80 eV. The value of the resistivity of the crystal Cd0.80Mn0.20Te is 2•107 Ohm • cm at the beginning of the ingot and decreases by 2 orders of magnitude by the end of the ingot.
Cd0.80Mn0.20Te固溶体的相平衡
本文研究了Cd0.80Mn0.20Te固溶体的热性能。合金的热成像采用了两种热处理方法,从而可以研究其热性能。样品的热成像方法之一是将样品加热到最高温度,并在此温度下保存一段时间,然后对样品进行冷却。用这种热像仪获得的数据可以得到表征熔体Cd0.80Mn0.20Te结晶参数的图形。结果表明,Cd0.80Mn0.20Te熔体在熔点温度低于14°С时无过冷结晶,为两相熔体。结果表明,Cd0.80Mn0.20Te熔体的结晶速率随结晶温度的降低而增大。合金热处理的第二种方法是在将样品加热到最高温度(1150℃)时进行一系列等温保温。因此,对合金的熔化参数进行了研究。结果表明,在1078 ~ 1095°С温度范围内,Cd0.80Mn0.20Te熔体固相体积分数由100%下降到0%。根据所获得的差热分析数据,在控制条件下生长出Cd0.80Mn0.20Te铸锭。切割这个晶体后,我们可以看到几个不同大小的单晶区域。红外显微镜观察发现,样品中直径<7 mm的夹杂物数量最少,分布在样品的不同部位,所有样品的带隙值在1.78 ~ 1.80 eV之间。晶体Cd0.80Mn0.20Te的电阻率在铸锭开始时为2•107欧姆•cm,在铸锭结束时降低了2个数量级。
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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