Three separate measurements are made on doped silicon samples.

PHYSICS · Multi-part · Fermi University Physics · Condensed Matter, Materials & Soft Matter · Electronic transport in solids · Semiconductor physics and devices

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

Problem

Three separate measurements are made on doped silicon samples. ((a)) A cyclotron resonance experiment at microwave frequency f=35.0 GHzf=35.0\,\mathrm{GHz} on p-type silicon shows two hole resonances, at B1=0.200 TB_1=0.200\,\mathrm{T} and B2=0.610 TB_2=0.610\,\mathrm{T}. Using m∗=eB/ωm^*=eB/\omega with ω=2πf\omega=2\pi f, calculate the two masses (in units of mem_e) and state which line is the heavy-hole line and which is the light-hole line. ((b)) A Hall carrier density nH(T)n_H(T) is measured on an n-type silicon sample with ND=2×1015 cm−3N_D=2\times10^{15}\,\mathrm{cm^{-3}}: nH=3×1014 cm−3n_H=3\times10^{14}\,\mathrm{cm^{-3}} at 60 K60\,\mathrm{K}, nH=2×1015 cm−3n_H=2\times10^{15}\,\mathrm{cm^{-3}} at 150 K150\,\mathrm{K}, and nH=1×1016 cm−3n_H=1\times10^{16}\,\mathrm{cm^{-3}} at 650 K650\,\mathrm{K}. Identify the regime (freeze-out, extrinsic or intrinsic) at each temperature, with a one-line reason for each. ((c)) An electron drift mobility μn(T)\mu_n(T) is measured on a doped silicon sample: μn=800 cm2 V−1s−1\mu_n=800\,\mathrm{cm^2\,V^{-1}s^{-1}} at 20 K20\,\mathrm{K}, μn=3160 cm2 V−1s−1\mu_n=3160\,\mathrm{cm^2\,V^{-1}s^{-1}} at 50 K50\,\mathrm{K}, μn=1450 cm2 V−1s−1\mu_n=1450\,\mathrm{cm^2\,V^{-1}s^{-1}} at 300 K300\,\mathrm{K}, and μn=670 cm2 V−1s−1\mu_n=670\,\mathrm{cm^2\,V^{-1}s^{-1}} at 500 K500\,\mathrm{K}. Using pairs of points on either side of the peak, estimate the power-law exponent nn in μn∝Tn\mu_n\propto T^n below and above 50 K50\,\mathrm{K}, and name the scattering mechanism responsible for each.

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