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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Some compounds with the zinc blende structure are listed in Table 1.9. The bonding is less ionic than in compounds with the rock salt structure. Thus, oxides do not usually have the zinc blende structure (ZnO, not included in Table 1.9, is an exception; it is dimorphic with zinc blende and wurtzite structure polymorphs). Chalcogenides of the alkaline earth metals (but not Be) have the rock salt structure, whereas the chalcogenides of Be, Zn, Cd, and Hg have the zinc blende structure, as do Cu(I) halides and Γ ‐AgI. A range of III–V compounds (i.e. elements from Groups III and V of the Periodic Table) have the zinc blende structure and some, e.g. GaAs, are important semiconductors.

Table 1.8 Some compounds with the NaCl structure, a/Å

MgO 4.213 MgS 5.200 LiF 4.0270 KF 5.347
CaO 4.8105 CaS 5.6948 LiCl 5.1396 KCl 6.2931
SrO 5.160 SrS 6.020 LiBr 5.5013 KBr 6.5966
BaO 5.539 BaS 6.386 LiI 6.00 KI 7.0655
TiO 4.177 α ‐MnS 5.224 LiH 4.083 RbF 5.6516
MnO 4.445 MgSe 5.462 NaF 4.64 RbCl 6.5810
FeO 4.307 CaSe 5.924 NaCl 5.6402 RbBr 6.889
CoO 4.260 SrSe 6.246 NaBr 5.9772 RbI 7.342
NiO 4.1769 BaSe 6.600 NaI 6.473 AgF 4.92
CdO 4.6953 CaTe 6.356 TiN 4.240 AgCl 5.549
TiC 4.3285 LaN 5.30 UN 4.890 AgBr 5.7745
Figure 133 The sphalerite zinc blende structure showing a the unit cell - фото 74

Figure 1.33 The sphalerite (zinc blende) structure showing (a) the unit cell contents and (b) a more extended network of corner‐sharing tetrahedra.

1.17.1.3 Antifluorite/fluorite structure

The antifluorite structure has ccp/fcc anions with cations in all (T +and T –) tetrahedral sites. The difference between antifluorite and fluorite is that antifluorite refers to an anion array with tetrahedral cations, whereas fluorite has the inverse arrangement with a ccp cation array and tetrahedral anions. Since the cation:anion ratio is 2:1 in antifluorite and the cation coordination is 4, the anion coordination must be 8, Fig. 1.30.

The very different coordination environments of anions and cations leads to two entirely distinct descriptions of the structure in terms of a 3D network of either tetrahedra or cubes, Fig. 1.34; (a) corresponds to the arrangement shown in Fig. 1.29(c) and the tetrahedra are highlighted; (b) corresponds to the arrangement in Fig. 1.30(b) in which the cubic coordination arrangement is highlighted. A more extended network of corner‐and edge‐sharing cubes is shown in Fig. 1.34(c). This must surely rate as one of the world's largest models of the antifluorite structure!

The antifluorite structure is shown by a large number of oxides and other chalcogenides of the alkali metals (Table 1.10), i.e. compounds of general formula картинка 75. A group of fluorides of large, divalent cations and oxides of large tetravalent cations have the inverse, fluorite, structure, i.e. M 2+F 2and M 4+O 2.

From Fig. 1.34(b) and (c), an alternative way of describing the fluorite structure is as a primitive cubic array of anions in which the eight‐coordinate sites at the cube body centres are alternately empty and occupied by a cation. It should be stressed that the true lattice type of fluorite is fcc and not primitive cubic, since the primitive cubes represent only a small part (one‐eighth) of the fcc unit cell. Description of fluorite as a primitive cubic array of anions with alternate cube body centres occupied by cations shows a similarity to the CsCl structure (see later). This also has a primitive cubic array of anions, but, instead, cations occupy all the body centre sites.

Table 1.9 Some compounds with the zinc blende (sphalerite) structure, a/Å

CuF 4.255 BeS 4.8624 β ‐CdS 5.818 BN 3.616 GaP 5.448
CuCl 5.416 BeSe 5.07 CdSe 6.077 BP 4.538 GaAs 5.6534
γ ‐CuBr 5.6905 BeTe 5.54 CdTe 6.481 BAs 4.777 GaSb 6.095
γ ‐CuI 6.051 β ‐ZnS 5.4060 HgS 5.8517 AlP 5.451 InP 5.869
γ ‐AgI 6.495 ZnSe 5.667 HgSe 6.085 AlAs 5.662 InAs 6.058
β ‐MnS, red 5.600 β ‐SiC 4.358 HgTe 6.453 AlSb 6.1347 InSb 6.4782
C a 3.5667 Si 5.4307 Ge 5.6574 α ‐Sn (grey) 6.4912

a Diamond structure.

Figure 134 The antifluorite structure of Na2O showing the unit cell in terms - фото 76

Figure 1.34 The antifluorite structure of Na2O showing the unit cell in terms of (a) NaO4 tetrahedra and (b) ONa8 cubes. A more extended array of cubes is shown in (c); this model resides on a roundabout in Mexico City.

Most fluorite structures are eutactic in terms of descriptions as both a primitive cubic array of anions and an fcc array of cations. Thus, the anions are usually too large to occupy tetrahedral holes in a fully dense ccp cation array and, conversely, cations are too large to occupy eight‐coordinate sites in a fully dense primitive cubic anion array. A compound that approaches maximum density is Li 2Te containing the smallest alkali metal and largest chalcogen and for which the Te–Te distance, 4.6 Å, is only slightly greater than the diameter of the Te 2+ion, 4.4 Å.

In this section, we have described the ideal cubic fluorite structure, A 2X. A number of closely related structures with a range of formulae, including the pyrochlore structure, is described in Section 1.17.12.

Table 1.10 Some compounds with fluorite or antifluorite structure, a/Å

Fluorite structure Antifluorite structure
CaF 2 5.4626 PbO 2 5.349 Li 2O 4.6114 K 2O 6.449
SrF 2 5.800 CeO 2 5.4110 Li 2S 5.710 K 2S 7.406
SrCl 2 6.9767 PrO 2 5.392 Li 2Se 6.002 K 2Se 7.692
BaF 2 6.2001 ThO 2 5.600 Li 2Te 6.517 K 2Te 8.168
CdF 2 5.3895 UO 2 5.372 Na 2O 5.55 Rb 2O 6.74
β ‐PbF 2 5.940 NpO 2 5.4334 Na 2S 6.539 Rb 2S 7.65

1.17.1.4 Cuprite structure, Cu2O

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