Get 20M+ Full-Text Papers For Less Than $1.50/day. Start a 14-Day Trial for You or Your Team.

Learn More →

Systematic errors in precision lattice-parameter determination of single crystals caused by asymmetric line profiles

Systematic errors in precision lattice-parameter determination of single crystals caused by... The convolution of the various contributions to X-ray intensity distribution curves measured in lattice-parameter determination leads to peak shifts and, hence, to systematic errors in the case that at least one of the contributing curves is asymmetric. For perfect crystals, depending on the collimator divergence, this effect may reach the order of magnitude of the refraction correction. It is caused by the asymmetry of the spectral distribution curve, which includes intrinsic asymmetry, dispersion and angle dependence of intensity (ADI). For imperfect crystals characterized by orientation and interplanar-spacing distributions, the distribution curves should be measured in order to correct accurately the peak shift. Examples of simulation calculations are given for Si, Cu K1, Bond method for various reflections of perfect crystals and for crystals having orientation distributions, 444 reflection. http://www.deepdyve.com/assets/images/DeepDyve-Logo-lg.png Journal of Applied Crystallography International Union of Crystallography

Systematic errors in precision lattice-parameter determination of single crystals caused by asymmetric line profiles

Journal of Applied Crystallography , Volume 19 (1): 34 – Feb 1, 1986

Systematic errors in precision lattice-parameter determination of single crystals caused by asymmetric line profiles

Journal of Applied Crystallography , Volume 19 (1): 34 – Feb 1, 1986

Abstract

The convolution of the various contributions to X-ray intensity distribution curves measured in lattice-parameter determination leads to peak shifts and, hence, to systematic errors in the case that at least one of the contributing curves is asymmetric. For perfect crystals, depending on the collimator divergence, this effect may reach the order of magnitude of the refraction correction. It is caused by the asymmetry of the spectral distribution curve, which includes intrinsic asymmetry, dispersion and angle dependence of intensity (ADI). For imperfect crystals characterized by orientation and interplanar-spacing distributions, the distribution curves should be measured in order to correct accurately the peak shift. Examples of simulation calculations are given for Si, Cu K1, Bond method for various reflections of perfect crystals and for crystals having orientation distributions, 444 reflection.

Loading next page...
 
/lp/international-union-of-crystallography/systematic-errors-in-precision-lattice-parameter-determination-of-wZJEzYCUd1

References (5)

Publisher
International Union of Crystallography
Copyright
Copyright (c) 1986 International Union of Crystallography
ISSN
0021-8898
DOI
10.1107/S0021889886090039
Publisher site
See Article on Publisher Site

Abstract

The convolution of the various contributions to X-ray intensity distribution curves measured in lattice-parameter determination leads to peak shifts and, hence, to systematic errors in the case that at least one of the contributing curves is asymmetric. For perfect crystals, depending on the collimator divergence, this effect may reach the order of magnitude of the refraction correction. It is caused by the asymmetry of the spectral distribution curve, which includes intrinsic asymmetry, dispersion and angle dependence of intensity (ADI). For imperfect crystals characterized by orientation and interplanar-spacing distributions, the distribution curves should be measured in order to correct accurately the peak shift. Examples of simulation calculations are given for Si, Cu K1, Bond method for various reflections of perfect crystals and for crystals having orientation distributions, 444 reflection.

Journal

Journal of Applied CrystallographyInternational Union of Crystallography

Published: Feb 1, 1986

There are no references for this article.