Electron Self-Energy and Temperature-Dependent Effective Masses in Semiconductors:<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>n</mml:mi></mml:math>-Type Ge and Si

Abstract

The electronic self-energy due to interaction with acoustic phonons is evaluated as a function of the electron propagation vector k, and a relation is established connecting the Sommerfeld-Bethe interaction constant with the energy band separation and effective masses. For nondegenerate prolate ellipsoidal energy surfaces of revolution, the self-energy depends linearly on the temperature $T$ at high temperatures and quadratically on $T$ at low temperatures, this behavior being substantiated by the experimental results of Macfarlane and Roberts. The temperature dependence of the principal effective masses ${m}_{i}(T)$ at high temperatures is given by ($i=l or t$) $\frac{{m}_{i}(0)}{{m}_{i}(T)}=1+(\frac{128\ensuremath{\pi}}{9\ensuremath{\rho}{h}^{3}s{\ensuremath{\Theta}}_{D}}){{m}_{i}}^{2}(0){\ensuremath{\alpha}}_{i}(E){〈{C}^{2}〉}_{\mathrm{Av}}T$ thus indicating a decrease in effective mass with rising temperatures. The result does not explain the deviation from the ${T}^{\ensuremath{-}\frac{3}{2}}$ law for the lattice mobility as observed by Morin and Maita. The percentage decrease at room temperature for each of the electron effective masses amounts to less than 1%. These results do not account fully for the possible change determined by Lax and Mavroides.