Solid solutions and order–disorder

Abstract

Introduction Disorder in a solid may arise from several different sources: (1) The periodicity may be broken by displacing atoms from their equilibrium positions in a nonperiodic fashion. These defects can be point defects, single atoms in wrong positions, missing atoms, or impurities; line defects, chains of missing, extra, or misplaced atoms, or dislocations; planar defects, twin planes, or sheets of missing atoms; or three-dimensional or structural disorder or lack of periodicity leading eventually to amorphization. (2) A solid solution or alloy may form by replacing one atom, more or less at random, by another with reasonably similar properties, for example, Mg, Fe substitution in olivines. (3) Substitutional disorder may occur when similar atoms ordered onto crystallographic sites at low temperature are partially or completely randomized at high temperature. This situation creates positional disorder but maintains overall stoichiometry. (4) Nonstoichiometry, namely, deviation from ideal atomic ratios, for example, Fe 0.97 O instead of FeO, creates another kind of disorder. (5) The orientation of polyhedra (octahedral tilting in perovskites, CO 3 orientation in carbonates) may lose long-range order. (6) Magnetic moments or electron spins may become disordered. These various types of disorder are frequently related. In all cases, the equilibrium degree of disorder increases with increasing temperature because of the balance of energy and entropy. In many substitutional solid solutions formed at high temperature, the disorder may decrease as temperature is lowered by one or both of two mechanisms: (1) The atoms may order into a superstructure.