= Solution
A perfectly clean two-dimensional system has sharply degenerate <Landau levels> and integer filling only at isolated fields for fixed density. Real disorder broadens each level into a band, with states localized in the tails and extended states near its centre. When the <chemical potential> moves through a localized region, changing field can change the occupation of those localized states without changing the number of conducting extended channels. The Hall conductance then remains $pe^2/h$ and the <Hall voltage> at fixed current remains $I_xh/(pe^2)$ over a finite field interval.
In the same regime, separated edge channels and localized bulk states suppress dissipative backscattering, so $\rho_{xx}$ is very small. At a transition the <chemical potential> reaches the next band of extended states; longitudinal conduction rises and the Hall conductance changes to another integer. This is a mobility-gap explanation: a plateau does not require the <density of states> itself to vanish, nor does it require the carrier density to grow linearly with field. Low <temperature>, sufficient mobility and suitable contacts are needed to resolve it.
This physical explanation is determined by the surviving question text. Particular measured plateau heights and widths cannot be quoted because the source graph is absent, as recorded in part (b).
Back to article page
