This paper is concerned with scaling limits in kinetic semiconductor models
. For the classical Vlasov-Poisson-Fokker-Planck equation and its quantum m
echanical counterpart, the Wigner-Poisson-Fokker-Planck equation, three dis
tinguished scaling regimes are presented. Using Hilbert and Chapman-Enskog
expansions, we derive two drift-diffusion type approximations. The test cas
e of a n(+) - n - n(+) diode reveals that different scaling regimes may be
present at the same time in different subregions of a semiconductor device.
Numerical simulations of the stationary solution illustrate the good appro
ximation of the kinetic solution by a drift-diffusion model and by a hybrid
(adaptive domain decomposition) model.