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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These structures have in common an hcp arrangement of anions and differ only in the positions of the cations, as follows:

wurtzite: T+ (or T–) sites occupied; T– (or T+), O empty

nickel arsenide: O sites occupied; T+, T– empty.

These structures are the hcp analogues of the ccp sphalerite and rock salt structures, respectively. Note that there is no hexagonal equivalent of the fluorite and antifluorite structures.

Both wurtzite and nickel arsenide have hexagonal symmetry and unit cells. A unit cell containing hcp anions is shown in Fig. 1.35(a). It is less easy to visualise and draw on paper than a cubic cell because of the γ angle of 120°. The unit cell contains two anions, one at the origin and one inside the cell:

Solid State Chemistry and its Applications - изображение 90

In Fig. 1.35(b) is shown a projection down c of the same structure. Close packed layers occur in the basal plane, i.e. at c = 0 (blue circles), at c = 1 (not shown) and at картинка 91(pink circles). The layer stacking arrangement is repeated every other layer … ABABA. … The contents of one unit cell are shown in (c). Dashed circles represent atoms at the top four corners of the unit cell, i.e. at c = 1.

Figure 135 The wurtzite and nickel arsenide structures ac the hexagonal - фото 92 Figure 135 The wurtzite and nickel arsenide structures ac the hexagonal - фото 93

Figure 1.35 The wurtzite and nickel arsenide structures: (a–c) the hexagonal unit cell of an hcp anion array; (d, e) interstitial sites in an hcp array; (f, g) structures of wurtzite and NiAs; (h, i) trigonal prismatic coordination of arsenic in NiAs; (j–l) models of the ZnS and NiAs structures showing the arrangement and linkages of the polyhedra.

In metals which have hcp structures, adjacent metal atoms are in contact, e.g. along a 1and a 2(≡ b ) edges of the unit cell (b, c). In eutactic cp ionic structures, however, the anions may be pushed apart by the cations in the interstitial sites. Assuming for the moment that the anions are in contact, then the hexagonal unit cell has a definite shape given by the ratio c / a = 1.633. This is because a is equal to the shortest distance X–X, i.e. the diameter of an anion, and c is equal to twice the vertical height of a tetrahedron comprising four anions. The ratio c / a may then be calculated by geometry (see Appendix C).

The interstitial sites available for cations in an hcp anion array are shown in Fig. 1.35(d) for the bottom half of the unit cell between c = 0 and картинка 94and in (e) for the top half of the unit cell. Since the cell contains two anions, there must be two each of T +, T –and O.

A detailed description of the sites that are occupied in wurtzite and NiAs is now given for completeness; such a degree of detail may, however, not be necessary to gain an overview of these two structures and is not compulsory reading! In Fig. 1.35(d), a T –site occurs along the c edge of the cell at height картинка 95above the anion at the origin. This T –site is coordinated to three anions at картинка 96and one anion at the corner, c = 0. The tetrahedron so formed, therefore, points downwards. The position of the T –site inside this tetrahedron is at the centre of gravity, i.e. at one‐quarter of the vertical distance from base to apex (see Appendix C). Since the apex and base are at c = 0 and картинка 97, this T –site is at картинка 98. In practice, the occupant of this T –site in the wurtzite structure may not be at exactly 0.375 c . For those structures which have been studied accurately, Table 1.12, values range from 0.345 to 0.385; the letter u represents the fractional c value.

Table 1.12 Some compounds with the wurtzite structure

Compound картинка 99 картинка 100 u c / a Compound картинка 101 картинка 102 u c / a
ZnO 3.2495 5.2069 0.345 1.602 AgI 4.580 7.494 1.636
ZnS 3.811 6.234 1.636 AlN 3.111 4.978 0.385 1.600
ZnSe 3.98 6.53 1.641 GaN 3.180 5.166 1.625
ZnTe 4.27 6.99 1.637 InN 3.533 5.693 1.611
BeO 2.698 4.380 0.378 1.623 TaN 3.05 4.94 1.620
CdS 4.1348 6.7490 1.632 NH 4F 4.39 7.02 0.365 1.600
CdSe 4.30 7.02 1.633 SiC 3.076 5.048 1.641
MnS 3.976 6.432 1.618 MnSe 4.12 6.72 1.631

R. W. G. Wyckoff, Crystal Structures , Vols 1 to 6, Wiley (1971).

The three anions at картинка 103that form the base of this T –site also form the base of a T +site shown in Fig. 1.35(e) centred at картинка 104. The apex of this tetrahedron is the anion at the top corner with coordinates 0, 0, 1. Another T +site at картинка 105is coordinated to three anions in the basal plane and an anion at картинка 106(d). The triangular base of this site, at c = 0, is shared with a T –site underneath (not shown) at картинка 107. The equivalent T –site that lies inside the unit cell is at картинка 108(e).

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