3.3. TRANSPORT AND SCATTERING 103
8.07.06.05.04.03.02.01.00.0
0.00 0.10 0.20 0.30 0.40 0.50 0.60 0.70 0.80 0.90 1.00Polar optical phonon emissionPolar optical phonon absorptionAcoustic phonon scatteringSCATTERING RATE(1012–1s)ENERGY (eV)10.09.0GaAs EXAMPLE
hωop = 36 meV thresholdFigure 3.9: Scattering rates due to acoustic and optical phonons for GaAs electrons at room
temperature.
withnthe free electron density. The scattering rate for an electron with energyEkand momen-
tumkcan be shown to be
W(k)=4πF(
2 k
λ) 2 [
1
1+(λ/ 2 k)^2]
F =
1
(
e^2
) 2
N(Ek)
32 k^4NI (3.3.21)
whereNIis the ionized impurity density. Note that ionized impurities (and the scattering pro-
cesses discussed here) do not alter the spin of the electron. ThusN(E)is the density of states
withoutcountingthespindegeneracy i.e it is half the usual density of states.