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International Tables for Crystallography (2006). Vol. C. ch. 7.4, pp. 653-665
https://doi.org/10.1107/97809553602060000607 |
Chapter 7.4. Correction of systematic errors
Contents
- 7.4. Correction of systematic errors (pp. 653-665) | html | pdf | chapter contents |
- 7.4.1. Absorption (p. 653) | html | pdf |
- 7.4.2. Thermal diffuse scattering (pp. 653-657) | html | pdf |
- 7.4.2.1. Glossary of symbols (pp. 653-654) | html | pdf |
- 7.4.2.2. TDS correction factor for X-rays (single crystals) (pp. 654-656) | html | pdf |
- 7.4.2.3. TDS correction factor for thermal neutrons (single crystals) (pp. 656-657) | html | pdf |
- 7.4.2.4. Correction factor for powders (p. 657) | html | pdf |
- 7.4.3. Compton scattering (pp. 657-661) | html | pdf |
- 7.4.3.1. Introduction (p. 657) | html | pdf |
- 7.4.3.2. Non-relativistic calculations of the incoherent scattering cross section (pp. 657-659) | html | pdf |
- 7.4.3.3. Relativistic treatment of incoherent scattering (pp. 659-660) | html | pdf |
- 7.4.3.4. Plasmon, Raman, and resonant Raman scattering (pp. 660-661) | html | pdf |
- 7.4.3.5. Magnetic scattering (p. 661) | html | pdf |
- 7.4.4. White radiation and other sources of background (pp. 661-665) | html | pdf |
- References | html | pdf |
- Figures
- Fig. 7.4.2.1. 060 reflection of LiNbO3 (Mössbauer diffraction) (p. 653) | html | pdf |
- Fig. 7.4.2.2. Diagrams in reciprocal space illustrating the volume abcd swept out for (a) an ω scan, and (b) a θ/2θ, or ω/2θ, scan (p. 655) | html | pdf |
- Fig. 7.4.2.3. Scattering surfaces for one-phonon scattering of neutrons: (a) for neutrons faster than sound (β < 1); (b) for neutrons slower than sound (β > 1) (p. 656) | html | pdf |
- Fig. 7.4.2.4. One-phonon scattering calculated for polycrystalline nickel of lattice constant a (after Suortti, 1980a) (p. 656) | html | pdf |
- Fig. 7.4.3.1. Schematic diagram of the inelastic scattering interactions, ΔE = E1 − E2 is the energy transferred from the photon and K the momentum transfer (p. 657) | html | pdf |
- Fig. 7.4.3.2. The incoherent scattering function, S(x, Z)/Z, per electron for aluminium shown as a function of x = (sin θ)/λ (p. 660) | html | pdf |
- Fig. 7.4.3.3. The cross section for resonant Raman scattering (RRS) and fluorescence (F) as a function of the ratio of the incident energy, E, and the K-binding energy, EB (p. 661) | html | pdf |
- Fig. 7.4.4.1. Equatorial phase-space diagrams for a conventional X-ray source and parallel-beam geometry; x is the size and x′ = dx/dz the divergence of the X-rays (p. 662) | html | pdf |
- Fig. 7.4.4.2. Reflection 400 of LiH measured with a parallel beam of Mo Kα1 radiation (solid curve) (p. 662) | html | pdf |
- Fig. 7.4.4.3. Equatorial phase-space diagrams for two wavelengths, λ1 (solid lines) and λ2 (broken lines), projected on the plane λ = λ1 (p. 662) | html | pdf |
- Fig. 7.4.4.4. Two reflections of beryllium acetate measured with Mo Kα (p. 663) | html | pdf |
- Fig. 7.4.4.5. Components of scattering at small scattering angles when the incident energy is just below the K absorption edge of the sample [upper part, (a)], and at large scattering angles when the incident energy is about twice the K-edge energy [upper part, (b)] (p. 663) | html | pdf |
- Fig. 7.4.4.6. Equatorial phase-space diagrams for powder diffraction in the Bragg–Brentano geometry (p. 664) | html | pdf |
- Fig. 7.4.4.7. Three measurements of the 220 reflection of Ni at λ = 1.541 Å scaled to the same peak value; (a) in linear scale, (b) in logarithmic scale (p. 664) | html | pdf |
- Tables
- Table 7.4.3.1. The energy transfer, in eV, in the Compton scattering process for selected X-ray energies (p. 657) | html | pdf |
- Table 7.4.3.2. The incoherent scattering function for elements up to Z = 55 (p. 658) | html | pdf |
- Table 7.4.3.3. Compton scattering of Mo Kα X-radiation through 170° from 2s electrons (p. 659) | html | pdf |