Anthony R. West - Solid State Chemistry and its Applications

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SOLID STATE CHEMISTRY AND ITS APPLICATIONS
A comprehensive treatment of solid state chemistry complete with supplementary material and full colour illustrations from a leading expert in the field. Solid State Chemistry and its Applications, Second Edition
Student Edition
Significant updates and new content in this second edition include:
A more extensive overview of important families of inorganic solids including spinels, perovskites, pyrochlores, garnets, Ruddlesden-Popper phases and many more New methods to synthesise inorganic solids, including sol-gel methods, combustion synthesis, atomic layer deposition, spray pyrolysis and microwave techniques Advances in electron microscopy, X-ray and electron spectroscopies New developments in electrical properties of materials, including high Tc superconductivity, lithium batteries, solid oxide fuel cells and smart windows Recent developments in optical properties, including fibre optics, solar cells and transparent conducting oxides Advances in magnetic properties including magnetoresistance and multiferroic materials Homogeneous and heterogeneous ceramics, characterization using impedance spectroscopy Thermoelectric materials, MXenes, low dimensional structures, memristors and many other functional materials Expanded coverage of glass, including metallic and fluoride glasses, cement and concrete, geopolymers, refractories and structural ceramics Overview of binary oxides of all the elements, their structures, properties and applications Featuring full color illustrations throughout, readers will also benefit from online supplementary materials including access to CrystalMaker® software and over 100 interactive crystal structure models.
Perfect for advanced students seeking a detailed treatment of solid state chemistry, this new edition of
will also earn a place as a desk reference in the libraries of experienced researchers in chemistry, crystallography, physics, and materials science.

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This structure is related to fluorite, CaF 2but only 1/4 of the tetrahedral positions are occupied by anions. Cu forms an fcc array; two tetrahedral sites, at 1/4, 1/4, 1/4 and 3/4, 3/4, 3/4, are occupied by O. Consequently, the CN of Cu is twofold linear, rather than 8‐fold for Ca in fluorite and 4‐fold for Zn in sphalerite. Another way to view the structure is as two interpenetrating lattices, fcc Cu and bcc O, giving a structure that, overall, is primitive cubic, a = 4.267 Å. The linear, or ‘dumbell’ coordination of 2 is unusual for a reasonably sized cation but is a common feature in structures of monovalent Cu 3 d 10and may be rationalised in terms of sp hybridisation giving two Cu sp hybrid orbitals, arranged linearly.

1.17.1.5 Bond length calculations

It is very often desirable to be able to calculate interatomic distances in crystal structures. This is usually straightforward for crystals which have orthogonal unit cells (i.e. α = β = γ = 90°), and involves simple trigonometric calculations. For example, in the rock salt structure, the anion‐cation distance is a /2 and the anion–anion distance is картинка 77. The main interatomic distances involving cations in T/O sites in an fcc/ccp anion array are shown in Fig. 1.25(c) and are summarised in Table 1.11 for the important structure types. These may be used together with the tables of unit cell dimensions, Table 1.9, etc., for calculations on specific compounds. Typical values of bond distances (to oxygen and fluorine) for all the elements are given in Appendix F, where relevant values for different coordination numbers and oxidation states are also given.

Consideration of atom arrangements in the three structure types described above shows that the concept of cp anions with cations in interstitial sites begins to break down in the fluorite structure. Thus, while the antifluorite structure of Na 2O may be regarded as containing ccp O 2–ions with Na +ions in tetrahedral sites, in the fluorite structure of CaF 2, it is necessary to regard the Ca 2+ions as forming the ccp array with F –ions in tetrahedral sites. In CaF 2the Ca 2+ions have a eutactic ccp arrangement, but are well separated from each other; from Table 1.9 and Table 1.10, Ca–Ca = 3.86 Å, which is much larger than the diameter of a Ca 2+ion (depending on which table of ionic radii is consulted, the diameter of Ca 2+is in the range ~2.2–2.6 Å).

The F–F distance in CaF 2is 2.73 Å, which indicates that the fluorines are approximately contacting Solid State Chemistry and its Applications - изображение 78. Although the array of F –ions in CaF 2is not cp but is primitive cubic, this is perhaps a more realistic way of describing the structure than as containing a eutactic ccp array of Ca 2+ions; nevertheless, both descriptions are used widely.

1.17.2 Diamond

This structure type, so important to the semiconductor industry, has already been described, as the zinc blende or sphalerite structure, Fig. 1.29 and Fig. 1.33. The diamond structure is obtained when the two elements in zinc blende are identical, as in diamond. It may therefore be described as a ccp array of carbon atoms, with one set of tetrahedral sites (either T +or T –) occupied also by carbon atoms. It is, however, rather artificial to make a distinction between packing and interstitial atoms since structurally they are identical. Most Group IV elements crystallise with the diamond structure, Table 1.9.

Table 1.11 Calculation of interatomic distances in some simple structures

Structure type Distance Number of such distances Magnitude of distance in terms of unit cell dimensions
Rock salt (cubic) Na–Cl 6 a /2 = 0.5 a
Cl–Cl 12 Solid State Chemistry and its Applications - изображение 79
Na–Na 12 Solid State Chemistry and its Applications - изображение 80
Zinc blende (cubic) Zn–S 4 Solid State Chemistry and its Applications - изображение 81
Zn–Zn 12 Solid State Chemistry and its Applications - изображение 82
S–S 12 Solid State Chemistry and its Applications - изображение 83
Fluorite (cubic) Ca–F 8 Solid State Chemistry and its Applications - изображение 84
Ca–Ca 12 Solid State Chemistry and its Applications - изображение 85
F–F 6 a /2 = 0.5 a
Wurtzite a (hexagonal) Zn–S 4 ZnZn 12 a 0612 c SS 12 a 0612 c Nickel arsenide a hexagonal - фото 86
Zn–Zn 12 a = 0.612 c
S–S 12 a = 0.612 c
Nickel arsenide a (hexagonal) Ni–As 6 AsAs 12 a 0612 c NiNi 2 c 2 05 c 0816 a NiNi 6 a - фото 87
As–As 12 a = 0.612 c
Ni–Ni 2 c /2 = 0.5 c = 0.816 a
Ni–Ni 6 a = 0.612 c
Caesium chloride (cubic) Cs–Cl 8 Solid State Chemistry and its Applications - изображение 88
Cs–Cs 6 a
Cl–Cl 6 a
Cadmium iodide (hexagonal) Cd–I 6 II 12 a 0612 c CdCd 6 a 0612 c a These formulae do not - фото 89
I–I 12 a = 0.612 c
Cd–Cd 6 a = 0.612 c

a These formulae do not necessarily apply when c/a is different from the ideal value of 1.633.

1.17.3 Wurtzite (ZnS) and nickel arsenide (NiAs)

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