A cyclotron resonance experiment on germanium at a fixed microwave frequency of

PHYSICS · Multi-part · Fermi University Physics · Condensed Matter, Materials & Soft Matter · Free electrons, energy bands and electronic structure · Semiconductor physics and devices

Solid State Physics, Ch Semiconductors: masses, statistics, defect levels and mobility

Problem

A cyclotron resonance experiment on germanium at a fixed microwave frequency of 24.0 GHz24.0\,\mathrm{GHz}, with the magnetic field along a crystal axis, shows two hole resonances as the field is swept, at B1=0.0369 TB_1=0.0369\,\mathrm{T} and B2=0.283 TB_2=0.283\,\mathrm{T}. ((a)) Compute the cyclotron mass m∗=eB/ωm^*=eB/\omega for each line and assign each to the heavy-hole or light-hole branch, given germanium's masses mhh=0.33 mem_{hh}=0.33\,m_e and mlh=0.043 mem_{lh}=0.043\,m_e. ((b)) A Hall measurement on a separate n-type germanium sample doped with ND=1.0×1014 cm−3N_D=1.0\times10^{14}\,\mathrm{cm^{-3}} of arsenic gives electron densities n=3.0×1012 cm−3n=3.0\times10^{12}\,\mathrm{cm^{-3}} at 40 K40\,\mathrm{K}, n=9.7×1013 cm−3n=9.7\times10^{13}\,\mathrm{cm^{-3}} at 120 K120\,\mathrm{K}, and n=5.0×1014 cm−3n=5.0\times10^{14}\,\mathrm{cm^{-3}} at 450 K450\,\mathrm{K}. Identify the regime (freeze-out, extrinsic or intrinsic) at each temperature, with your reasoning. ((c)) The same sample's electron mobility is measured as 9.0×103 cm2 V−1s−19.0\times10^{3}\,\mathrm{cm^2\,V^{-1}s^{-1}} at 20 K20\,\mathrm{K}, rising to a maximum of 5.0×104 cm2 V−1s−15.0\times10^{4}\,\mathrm{cm^2\,V^{-1}s^{-1}} at 60 K60\,\mathrm{K}, then falling to 3.9×103 cm2 V−1s−13.9\times10^{3}\,\mathrm{cm^2\,V^{-1}s^{-1}} at 300 K300\,\mathrm{K}. State which scattering mechanism dominates on each side of the maximum and the power law expected for each.

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