Abstract
Using a new method based on hot‐electron generation, band‐to‐band Auger recombination in n+ silicon is studied experimentally. Using the theory developed in Part I, a conservative analysis demonstrates that this Auger recombination is limited to an electron Auger coefficient smaller than 5×1032 cm6/sec which is in disagreement with some earlier studies reporting Cn =2.8×1031 cm6/sec.