An impurity atom in a solid has just two accessible states

PHYSICS · Multi-part · Fermi University Physics · Thermal, Statistical & Complex Systems · Condensed Matter, Materials & Soft Matter · Lattice dynamics and thermal properties of solids

Thermal Physics, Ch Two-level systems, paramagnets and the Einstein solid

Problem

An impurity atom in a solid has just two accessible states, the lower taken as zero energy and the upper at ε=0.040 eV\varepsilon = 0.040\,\mathrm{eV}. Take 1 eV=1.602×10−19 J1\,\mathrm{eV} = 1.602\times10^{-19}\,\mathrm{J}. The impurities are in equilibrium with the host lattice, which acts as a reservoir. ((a)) Find the heat capacity of one impurity at T=250 KT = 250\,\mathrm{K}, as a multiple of kBk_B. ((b)) Aluminium is described by the Einstein model with θE=320 K\theta_E = 320\,\mathrm{K}. Find CV/3NkBC_V/3Nk_B at 400 K400\,\mathrm{K}, and state by what percentage the lattice heat capacity still falls short of 3NkB3Nk_B.

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