用γ射线衍射法表征大单晶的完美性

Jochen R. Schneider, Hans A. Graf
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引用次数: 0

摘要

能量为400 keV的γ辐射的布拉格衍射实验允许对大单晶的体性质进行高分辨率的研究,这与生长单晶的表征以及结构相变的研究有关。这种辐射在物质中的吸收很弱,例如铜中的平均自由程为μo−1⋍1 cm。因此,样品可以安装在任何低温恒温器,炉或高压设备,而不会造成窗口问题。Bragg角仅为1°数量级,因此所测衍射轮廓的形状主要受晶格倾角的影响。γ射线衍射法是对背散射技术的补充,背散射技术最适合于晶格参数的测量。采用双晶设置衍射图案被记录与角分辨率为1弧秒。综合反射功率的绝对测量精度为1%或更高,通过使用0.02至0.04 Å范围内的各种波长,可以通过波长外推技术从不完美的单晶中确定高精度,与模型无关的结构因子。由于波长较短,偏振效应可以忽略不计。根据动态衍射理论预测的完美晶体衍射图的半最大值全宽一般小于0.5弧秒,消光长度约为0.5 mm。因此,来自完美晶格的微小畸变会导致测量到的综合反射能力发生相当大的变化。最近,可以用316和468 keV γ射线在Si中测量Pendellösung强度节拍,从而以±- 0.1%的精度确定220结构因子。此外,在浮区生长的Si晶体中观察到令人惊讶的各向异性应变场。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Characterization of the perfection of large single crystals by means of γ-ray diffractometry

Bragg diffraction experiments with γ-radiation of energies of the order of 400 keV allow for high resolution studies of bulk properties of large single crystals which are relevance for the characterization of as grown single crystals as well as for the investigation of structural phase transitions. The absorption of this radiation in matter is very weak, as an example, the mean free path in copper is μo−1 ⋍ 1 cm. Therefore samples can be mounted in any cryostat, furnace or high pressure device without causing window problems. The Bragg angles are only of the order of 1° and thus the shape of the measured diffraction profile is mainly affected by lattice tilts. γ-ray diffractometry is complementary to back scattering techniques which are most suitable for lattice parameter measurements. Using a double crystal setting diffraction patterns are recorded with an angular resolution of 1 second of arc. The integrated reflecting power is measured absolutely with an accuracy of 1% or better and by using various wave lengths in the range between 0.02 and 0.04 Å, highly accurate, model independent structure factors can be determined from imperfect single crystals by means of wave length extrapolation techniques. Because of the short wave length polarization effects are neglibible. The full width at half maximum of the diffraction pattern of a perfect crystal as predicted by dynamical diffraction theory is generally less than 0.5 seconds of arc and the extinction length is of the order of 0.5 mm. Therefore small distortions from a perfect lattice cause rather large changes in the measured integrated reflecting power. Recently Pendellösung intensity beats could be measured in Si with 316 and 468 keV γ-radiation allowing to determine the 220 structure factor with an accuracy of ±- 0.1 %. In addition a surprisingly anisotropic strain field has been observed in floating-zone grown Si crystals.

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