Abstract
Hot electron transport is studied in small semiconductor structures by solving the coupled Boltzmann and Poisson equations using a simple relaxation time model and the integral formulation of the transport equation. Especially ballistic transport is investigated by calculating the electron distribution function f(x, v) in a submicron n+−n−−n+ diode. In the n−‐region f(x, v) is non‐Maxwellian and the ballistic electrons cause a dominant peak in f(x, v). The validity of the relaxation time approximation (RTA) is studied in the case of a large homogeneous electric field by calculating f(x, v) both, in RTA and using the full scattering rates for polar optical phonon scattering.
| Original language | English |
|---|---|
| Pages (from-to) | 827-835 |
| Journal | Physica Status Solidi B: Basic Research |
| Volume | 159 |
| Issue number | 2 |
| DOIs | |
| Publication status | Published - 1990 |
| MoE publication type | A1 Journal article-refereed |
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