Abstract:
The Landauer resistance $\rho_N^L$ has been generalized to the case of multichannel scattering of a particle by the system of $N$ nonoverlapping random potentials that are localized at the points $\xi$ ($i$ = 1, 2, $\dots$, $N$) and depend on $x$–$x_i$ and $y$. It has been shown that, in this case, a new resistance $\rho_N^S$ appears, which is an exponential function of $N$. The recurrence equation for determining the Landauer resistance $\rho_N^L$ has been derived and its solution in the general case has been obtained.