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多晶ZnSe、ZnS、CdTe、CaF₂和BaF₂、单晶KCl以及TI-20玻璃的红外热光系数测量

Infrared thermooptic coefficient measurement of polycrystalline ZnSe, ZnS, CdTe, CaF(2), and BaF(2), single crystal KCI, and TI-20 glass.

作者信息

Harris R J, Johnston G T, Kepple G A, Krok P C, Mukai H

出版信息

Appl Opt. 1977 Feb 1;16(2):436-8. doi: 10.1364/AO.16.000436.

Abstract

An interferometric technique has been used to determine the thermooptic coefficient (dn/dT) of polycrystalline ZnSe and ZnS at 0.6328 microm, 1.15 microm, 3.39 microm, and 10.6 microm; polycrystalline CdTe and TI-20 glass at 1.15 microm, 3.39 microm, and 10.6 microm; polycrystalline CaF(2) and BaF(2) at 0.6328 microm, 1.15 microm, and 3.39 microm, and pure and europium-doped single crystal KCl at 0.6328 microm, 1.15microm, 3.39 microm, and 10.6 microm. The values were obtained over the temperature range of 25-65 degrees C and were calculated using the observed change in optical path of the samples as they were heated. Some difficulties in thermometry were encountered in the standard configuration of sample and thermocouple probe, so measurements were made in an oil bath at the shortest wavelength at which the sample was transparent to provide temperature correction factors for each sample. An empirical dispersion relation for dn/dT has also been found for the semiconductor materials. This dispersion relation is of the form dn/dT = aR(b), where R is defined as lambda(2)/(lambda(2) - lambda(g)(2)), lambda(g) is the short wavelength cutoff associated with the energy gap, and a and b are constants which are different for each material.

摘要

一种干涉测量技术已被用于测定多晶ZnSe和ZnS在0.6328微米、1.15微米、3.39微米和10.6微米处的热光系数(dn/dT);多晶CdTe和TI-20玻璃在1.15微米、3.39微米和10.6微米处的热光系数;多晶CaF₂和BaF₂在0.6328微米、1.15微米和3.39微米处的热光系数,以及纯的和铕掺杂的单晶KCl在0.6328微米、1.15微米、3.39微米和10.6微米处的热光系数。这些值是在25至65摄氏度的温度范围内获得的,并利用样品加热时观察到的光程变化进行计算。在样品和热电偶探头的标准配置中遇到了一些温度测量方面的困难,因此在油浴中以样品透明的最短波长进行测量,以提供每个样品的温度校正因子。还发现了半导体材料dn/dT的经验色散关系。这种色散关系的形式为dn/dT = aR(b),其中R定义为λ²/(λ² - λg²),λg是与能隙相关的短波长截止值,a和b是每种材料不同的常数。

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