Localization properties of quasi-one dimensional quantum wire nanostructures
are investigated using the transfer matrix-Lyapunov exponent technique. We
calculate the localization length as a function of the effective mean-field
mobility assuming the random disorder potential to be arising from
dopant-induced short-range δ-function or finite-range Gaussian impurity
scattering. The localization length increases approximately linearly with the
effective mobility, and is also enhanced by finite-range disorder. There is a
sharp reduction in the localization length when the chemical potential crosses
into the second subband.Comment: 4 pages, RevTeX 3.0, 5 figures (available upon request