Caesium chloride crystallises as a simple cubic lattice with a two-ion basis, Cs at…

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

Caesium chloride crystallises as a simple cubic lattice with a two-ion basis, Cs+^+ at (0,0,0)(0,0,0) and Cl−^- at (12,12,12)(\tfrac12,\tfrac12,\tfrac12). Unlike bcc, the two basis positions are occupied by different ions, so the lattice itself is simple cubic, not body-centred. Using form factors fCsf_{\rm Cs} and fClf_{\rm Cl}, derive SGS_{\mathbf{G}} and show that, unlike bcc, no reflection is ever exactly extinguished. Then find the intensity ratio I100/I110I_{100}/I_{110}, taking fCs=55f_{\rm Cs}=55 and fCl=17f_{\rm Cl}=17 at zero angle, their electron counts.

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