修正最大熵法在低对称多晶聚集体QTA中的应用

Y. D. Wang, J. Z. Xu, Z. Liang
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引用次数: 4

摘要

提出了一种新的定量织构分析(QTA)算法,称为修正最大熵法(MMEM),并将其应用于衍射峰重叠的低晶对称多晶样品的织构测定(Wang and Xu, 1995a)。通过将最大熵原理直接引入到极点图反演的最小二乘过程中(Bunge, 1969),可以同时满足实验极点图数据与假设极点图数据之间差异的最小化和熵的最大化。因此,将最大熵原理应用于谐波法框架下QTA的整个过程。以模拟纤维纹理为例,对传统的最大熵法(HM)、最大熵法(MEM)和最大熵法(MMEM)三种极图反演方法进行了详细的比较。结果表明,对于具有光滑或尖锐纹理的多晶样品,即使使用较少的极点图,MMEM也能得到精确而稳定的反极点图解。详细讨论了MMEM对拟四边形材料进行QTA时所需要的最小极角范围和最小极位数。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The Modified Maximum Entropy Method (MMEM) in QTA for Lower Symmetry Polycrystalline Aggregates
A new algorithm of quantitative texture analysis (QTA), which is called the modified maximum entropy method (MMEM), has been proposed and applied to determination of textures in polycrystalline samples of lower crystal symmetry with overlapping diffraction peaks (Wang and Xu, 1995a). By introducing directly the maximum entropy principle into the least square procedure of pole figure inversion (Bunge, 1969), then both minimizing the differences between experimental and postulated pole figure data, and maximizing entropy may be satisfied simultaneously. Thus, the maximum entropy principle is applied to the entire process of QTA in frame of the harmonic method (HM). The detailed comparisons among the three pole figure inversion methods, i.e. the traditional HM, the primary maximum entropy method (MEM) and the MMEM, are given through a model example of simulated fiber texture. It is shown that the precise and stable solution of inverse pole figure for the polycrystalline samples with smooth or sharp textures will be obtained by the MMEM even using a less number of pole figures. The minimum range of polar angle and the least number of pole figures, which are needed in the QTA for pretended tetragonal materials by the MMEM, are discussed in detail.
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