Abstract
A calculation of the conductance of a metal-semiconductor tunnel junction for which interactions with optical phonons occur in the semiconductor electrode is given. The calculation is based upon a Green's-function theory of Appelbaum, Brinkman, and Zawadowski. The conductance is found for a uniform self-energy and a spatially dependent self-energy. Although there is qualitative agreement between the present results and the main features of the transfer Hamiltonian formalism given by Davis and Duke, further analysis of the data on pSi indicates that barrier effects occur in addition to the electrode effects. On the basis of the doping dependence of the reverse-bias line shape in pSi, it is suggested that a region of strong interaction with the optical phonons occurs in the barrier near the metal electrode at low doping levels.