A crystal of a single element

PHYSICS · Subjective · Fermi University Physics · Condensed Matter, Materials & Soft Matter · Crystal structure, bonding and diffraction · Crystal structure, bonding and diffraction

Condensed Matter Physics, Ch Diffraction: how a structure is actually measured

Problem

A crystal of a single element, known to be cubic, gives a powder pattern (Cu Kα1\alpha_1, λ=1.5406 A˚\lambda=1.5406\,\mathrm{\mathring{A}}) with lines at 2θ=23.732\theta=23.73, 39.2439.24, 46.3746.37, 56.7056.70, 62.3262.32 and 71.1271.12 degrees, and no others below 7272 degrees. Its measured density is 5.77 g cm−35.77\,\mathrm{g\,cm^{-3}} and its molar mass is 118.71 g mol−1118.71\,\mathrm{g\,mol^{-1}}. (a) Show from the ratios of sin⁡2θ\sin^2\theta that the lattice is neither simple cubic nor body-centred cubic. (b) Decide between a face-centred cubic lattice with one atom at each lattice point and the diamond structure, using both the lines that are missing and the density; then index the six lines and find aa to four figures.

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