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首页> 外文期刊>Journal of Applied Physics >Experimental and theoretical study of bulk light scattering in CaF_2 monocrystals
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Experimental and theoretical study of bulk light scattering in CaF_2 monocrystals

机译:CaF_2单晶中体光散射的实验和理论研究

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A variety of different types of light scattering (Rayleigh, Brillouin, Raman, and Mie scatterings), which may contribute to the transmission losses in the bulk of high-quality CaF_2 monocrystals, have been investigated experimentally and theoretically. The angular distribution of Rayleigh and Mie scatterings in the visible spectral range has been measured using an imaging technique. An effective technique for scattering measurements in the uv spectral range has also been implemented. Measurement of Raman scattering has shown that its contribution to the total scattering loss is negligible. In order to estimate the scattering from thermal fluctuations versus that from crystalline defects, a measurement of the temperature dependence of the scattering at the scattering angle of 90° has been performed. It has been shown that scatterings from thermal fluctuations and defects are of the same order of magnitude. Taking into account the dependence of the Brillouin scattering on the direction of the incident beam relative to crystalline axes, an upper limit of scattering loss due to thermal fluctuation in the perfect crystal has been evaluated theoretically. At 193 nm this limit appeared to be 2.6 X 10~(-5) cm~(-1), which is about two orders of magnitude less than the scattering loss in fused silica. Measured values of Rayleigh and Mie scatterings are in reasonable agreement with theoretical evaluation. Scattering measured in high-quality samples are comparable with the scattering calculated from thermodynamic fluctuations, indicating that the transmission of these samples is approaching the theoretical limit.
机译:已经通过实验和理论研究了各种不同类型的光散射(瑞利,布里渊,拉曼和米氏散射),这些光散射可能会导致大量高质量CaF_2单晶的透射损耗。已经使用成像技术测量了可见光谱范围内的瑞利和米氏散射的角分布。还已经实施了一种用于在紫外光谱范围内散射测量的有效技术。拉曼散射的测量表明,其对总散射损耗的贡献可忽略不计。为了估计来自热波动的散射与来自晶体缺陷的散射,从散射角度为90°的散射的温度依赖性进行了测量。已经表明,由热波动和缺陷引起的散射具有相同的数量级。考虑到布里渊散射对入射光束相对于晶轴的方向的依赖性,理论上已经评估了由于完美晶体中的热波动而引起的散射损耗的上限。在193 nm处,该极限为2.6 X 10〜(-5)cm〜(-1),比熔融石英的散射损失小大约两个数量级。瑞利和米氏散射的测量值与理论评估合理吻合。在高质量样品中测得的散射与通过热力学波动计算出的散射可比,表明这些样品的透射率已接近理论极限。

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