A silicon crystal doped with a single donor species (no acceptors) is measured over a…

PHYSICS · Subjective · Fermi University Physics · Condensed Matter, Materials & Soft Matter · Semiconductor physics and devices · Semiconductor physics and devices

Condensed Matter Physics, Ch Homogeneous semiconductors: counting carriers, doping and mobility

Problem

A silicon crystal doped with a single donor species (no acceptors) is measured over a wide temperature range, giving the electron densities below (ignore the slow T3/2T^{3/2} prefactor within each sloped region, as the chapter does). Data: T=40 KT=40\,\mathrm{K}, n=2.58×1013 cm−3n=2.58\times10^{13}\,\mathrm{cm^{-3}}; T=50 KT=50\,\mathrm{K}, n=1.23×1014 cm−3n=1.23\times10^{14}\,\mathrm{cm^{-3}}; T=250 KT=250\,\mathrm{K}, n=2.00×1015 cm−3n=2.00\times10^{15}\,\mathrm{cm^{-3}}; T=750 KT=750\,\mathrm{K}, n=5.52×1015 cm−3n=5.52\times10^{15}\,\mathrm{cm^{-3}}; T=800 KT=800\,\mathrm{K}, n=8.65×1015 cm−3n=8.65\times10^{15}\,\mathrm{cm^{-3}}. Identify which regime each row belongs to, and use the 40 K40\,\mathrm{K} and 50 K50\,\mathrm{K} points to find the donor energy EdE_d, and the 750 K750\,\mathrm{K} and 800 K800\,\mathrm{K} points to find the gap EgE_g (there nn is only a few times its plateau value, so the doping cannot be ignored).

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