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International Tables for Crystallography (2019). Vol. H. ch. 7.13, pp. 868-884
https://doi.org/10.1107/97809553602060000987 |
Chapter 7.13. Powder diffraction of superconductors
Contents
- 7.13. Powder diffraction of superconductors (pp. 868-884) | html | pdf | chapter contents |
- 7.13.1. Introduction (pp. 868-870) | html | pdf |
- 7.13.2. Advantages of structure analysis from powder diffraction (pp. 870-872) | html | pdf |
- 7.13.3. Analysis of the chemical and structural features of nonstoichiometric superconductors (pp. 872-878) | html | pdf |
- 7.13.4. Magnetic order in superconductors and parent compounds (pp. 878-879) | html | pdf |
- 7.13.5. Conclusions (p. 879) | html | pdf |
- Appendix 7.13.1. The study of long-range magnetic order in superconductors (pp. 879-882) | html | pdf |
- References | html | pdf |
- Figures
- Fig. 7.13.1. Definitions of superconductivity (p. 868) | html | pdf |
- Fig. 7.13.2. Typical structures for higher-Tc superconducting compounds shown in Table 7.13.1 (p. 870) | html | pdf |
- Fig. 7.13.3. Definition of the vectors relevant in the evaluation of the magnetic structure factor (p. 871) | html | pdf |
- Fig. 7.13.4. Angular dependence of the atomic scattering amplitudes of iron for X-rays [fx(Fe)] and neutrons [b(Fe)], and of the magnetic form factors for Fe2+ [fM(Fe2+)] and Fe3+ [fM(Fe3+)] (p. 871) | html | pdf |
- Fig. 7.13.5. Schematic representation of the choice of radiation recommended for powder-diffraction experiments to obtain different structural information in research on superconductivity (p. 872) | html | pdf |
- Fig. 7.13.6. Schematic view of charge transfer between the conduction layer and the charge-reservoir layer in superconducting and related compounds (p. 872) | html | pdf |
- Fig. 7.13.7. Calculated atomic valence for Cu in the CuO2 plane layer versus oxygen content in the chain layer of YBa2Cu3O7−x (p. 873) | html | pdf |
- Fig. 7.13.8. Schematic layer-stacking structures of (a) (R1−xMx)2CuO4 and (b) HgBa2CuO4+x indicating the charge transfer between the reservoir and superconducting layers (p. 873) | html | pdf |
- Fig. 7.13.9. (a) Schematic view of electron transfer in Fe-based superconducting and related compounds (p. 874) | html | pdf |
- Fig. 7.13.10. Layers in copper-oxide high-Tc superconductors (p. 875) | html | pdf |
- Fig. 7.13.11. Structure stacking along the c axis for the HgBa2Can−1CunO2(n+2)+x series of superconductors (p. 876) | html | pdf |
- Fig. 7.13.12. Schematic plot of the possible diffraction peaks with consideration of the primitive lattice only (p. 877) | html | pdf |
- Fig. 7.13.13. A structural transformation induced by a rotation of the octahedra in the perovskite structure (p. 877) | html | pdf |
- Fig. 7.13.14. Structural transformation from tetragonal P4/mmm symmetry to orthorhombic Pmmm symmetry due to oxygen vacancy ordering in the CuO1−x charge-reservoir layer (p. 878) | html | pdf |
- Fig. 7.13.15. Possible vacancy-ordering arrangements in the Fe plane for AxFe2−ySe2 (p. 878) | html | pdf |
- Fig. 7.13.16. Representation of selected commensurate ferromagnetic and antiferromagnetic ordering schemes (p. 879) | html | pdf |
- Fig. 7.13.17. Types of magnetic lattices (p. 880) | html | pdf |
- Fig. 7.13.18. Selected magnetic symmetry and antisymmetry elements that Dannay et al (p. 881) | html | pdf |
- Fig. 7.13.19. Observed (crosses) and calculated (solid line) intensities of neutron powder diffraction intensity data for the superconductor NaFeAs at 5 K (p. 882) | html | pdf |
- Tables
- Table 7.13.1. Selected superconducting elements, alloys, intermetallics, copper oxides, iron-based compounds and others (p. 869) | html | pdf |
- Table 7.13.2. Selected layered copper-oxide superconductors (p. 875) | html | pdf |
- Table 7.13.3. Crystal systems, conventional coordinate systems and the 36 magnetic lattices in three dimensions (p. 880) | html | pdf |
- Table 7.13.4. Integral reflection conditions of centred magnetic lattices corresponding to Fig. 7.13.17 (p. 882) | html | pdf |