The limitations on carrier (holes and electrons)
drift due to high-field streamlining also randomly velocity vector
in equilibrium is reported. Asymmetrical distribution function
that converts randomness in zero-field to streamlined one in a
very high electric field is employed. The ultimate drift velocity is
found to be appropriate thermal velocity for a given
dimensionality for non-degenerately doped nanostructure.
However, the ultimate drift velocity is the Fermi velocity for
degenerately doped nanostructures. Quantum and high-field
effects controlling the transport of carrier in nanostructures are
described. The results obtained are applied to the modeling of a
nanowire transistor.
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The limitations on carrier (holes and electrons)
drift due to high-field streamlining also randomly velocity vector
in equilibrium is reported. Asymmetrical distribution function
that converts randomness in zero-field to streamlined one in a
very high electric field is employed. The ultimate drift velocity is
found to be appropriate thermal velocity for a given
dimensionality for non-degenerately doped nanostructure.
However, the ultimate drift velocity is the Fermi velocity for
degenera...
»