Annotation
Peynman's method of continual integration is applied to an electron in a random field; the ranges of application of the various approximations are elucidated. Green's functions and the state density are calculated with quantum corrections.
© 2016 Publisher M.V.Lomonosov Moscow State University
Authors
V.L. Bonch-Bruevich and A.G. Mironov
Semiconductor Physics Department
Semiconductor Physics Department