International
Tables for
Crystallography
Volume C
Mathematical, physical and chemical tables
Edited by E. Prince

International Tables for Crystallography (2006). Vol. C. ch. 2.2, p. 37

Section 2.2.7.1. General

J. R. Helliwella

a Department of Chemistry, University of Manchester, Manchester M13 9PL, England

2.2.7.1. General

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The tools required for making the necessary measurement of reflection intensities include

  • (a) beam-conditioning items;

  • (b) crystal goniostat;

  • (c) detectors.

In this section, we describe the common configurations for defining precise states of the X-ray beam. The topic of detectors is dealt with in Part 7 (see especially Section 7.1.6[link] ). The impact of detector distortions on diffraction geometry is dealt with in Subsection 2.2.7.4[link].

Within the topic of beam conditioning the following subtopics are dealt with:

  • – collimation;

  • – monochromators;

  • – mirrors.

An exhaustive survey is not given, since a wide range of configurations is feasible. Instead, the commonest arrangements are covered. In addition, conventional X-ray sources are separated from synchrotron X-ray sources. The important difference in the treatment of the two types of source is that on the synchrotron the position and angle of the photon emission from the relativistic charged particles are correlated. One result of this, for example, is that after monochromatization of the synchrotron radiation (SR) the wavelength and angular direction of a photon are correlated.

The angular reflecting range and diffraction-spot size are determined by the physical state of the beam and the sample. Hence, the idealized situation considered earlier of a point sample and zero-divergence beam will be relaxed. Moreover, the effects of the detector-imaging characteristics are considered, i.e. obliquity, parallax, point-spread factor, and spatial distortions.








































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