Chemistry · Ch 6 — Solid State
Imperfection in Solids
Imperfection in Solids
No real crystal is perfect -- the law of nature guarantees that every crystal carries some defects in the arrangement of its constituent particles. Far from being a flaw to be ignored, these defects have real, measurable consequences for a solid's physical and chemical properties, and even drive some of the most important technological uses of solids: doping (deliberately introducing a controlled crystal imperfection) is what increases the electrical conductivity of a semiconductor such as silicon, and the ability of a ferromagnetic material such as iron or nickel to be magnetised and demagnetised likewise depends on the presence of imperfections in its crystal structure.
Crystal defects are classified into four broad types: 1) point defects, 2) line defects, 3) interstitial defects, and 4) volume defects. This unit concentrates specifically on point defects, and more specifically still on point defects in ionic solids, which are further classified into three families: stoichiometric defects (Schottky and Frenkel defects), non-stoichiometric defects (metal excess and metal deficiency defects), and impurity defects. …
What this figure shows. A flowchart headed 'Point defects' branching into three boxes -- 'stiochiometric defects' [sic], 'non-stiochiometric defects' [sic] and 'impurity defects' -- with the stoichiometric-defects box branching further down into 'Schottky defect' and 'Frenkel defect', and the non-stoichiometric-defects box branching down into 'metal excess defect' and 'metal deficiency defect'. This chart is the roadmap for the whole of Section 6.7: it shows at a glance that 'point defect' is the umbrella term, that stoichiometric defects are the two where the crystal's overall formula stays fixed (Schottky, Frenkel), and that non-stoichiometric defects are the two where the cation:anion ratio genuinely shifts away from the ideal formula (metal excess, metal deficiency), with imp …