A single crystal of aluminium (fcc

PHYSICS · Multi-part · Fermi University Physics · Condensed Matter, Materials & Soft Matter · Crystal structure, bonding and diffraction · Lattice dynamics and thermal properties of solids

Solid State Physics, Ch Diffraction as measurement: form factors, thermal motion and refinement

Problem

A single crystal of aluminium (fcc, conventional cubic lattice constant a=4.05 A˚a=4.05\,\mathrm{\AA}, Debye temperature ΘD=428 K\Theta_D=428\,\mathrm{K}, molar mass 26.98 g mol−126.98\,\mathrm{g\,mol^{-1}}) is heated from 300 K300\,\mathrm{K} to 900 K900\,\mathrm{K}. Treat the atomic displacements as harmonic and Gaussian, so that 2W=⟨ux2⟩Q22W=\langle u_x^2\rangle Q^2 for this cubic crystal, and use the Debye estimate ⟨ux2⟩=3ℏ2T/(MkBΘD2)\langle u_x^2\rangle=3\hbar^2T/(Mk_B\Theta_D^2) per axis at each temperature. ((a)) Estimate the percentage of the (220)(220) Bragg intensity that has moved into the diffuse background between 300 K300\,\mathrm{K} and 900 K900\,\mathrm{K}. ((b)) A laboratory source delivers Cu Kα\mathrm{Cu\,K}\alpha X-rays, for which the linear attenuation coefficient of aluminium is μX=130 cm−1\mu_X=130\,\mathrm{cm^{-1}}. Thermal neutrons have an attenuation length of 100 mm100\,\mathrm{mm} in aluminium. Estimate the factor by which a neutron beam penetrates further into the crystal than the X-ray beam, and say briefly why this matters for measuring the weak diffuse background.

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