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. 2015 Jun 19;5:11467. doi: 10.1038/srep11467

Table 1. Two-dimensional electron (hole) density in the accumulation layer, Ns; corresponding two-dimensional charge carrier (electrons or holes) gas Fermi wavelength, kF; the transport relaxation time at the Fermi energy, τ(EF); and electron (hole) mobility, μ, for different values of the incline angle θ and donor concentration Nd0 = 1017 cm-3.

Incline angle θ π/2 π/4 π/8 π/16 π/32
Ns, 1014 cm−2 4.742(a)/9.137(b) 3.347/6.351 1.806/3.258 0.918/1.487 0.460/0.514
kF, 107 cm−1 5.458/7.577 4.586/6.317 3.369/4.524 2.401/3.057 1.701/1.798
τ(EF), 10−9 s 2.960/0.189 1.768/0.114 0.694/0.045 0.233/0.015 0.074/0.003
μ, 106 cm2/(Vs) 32.527/1.038 19.428/0.628 7.621/0.249 2.557/0.083 0.815/0.019

(a)Calculated for the head-to-head wall (charge carriers – electrons);

(b)Calculated for the tail-to-tail wall (charge carriers – holes).