Abstract
The space distribution of the Hall current in the two-dimensional system is investigated using the one-electron form of the Kubo linear response theory. The calculation confirms that the quantised Hall current is localised only at edges of the sample when the Fermi energy lies in a gap between Landau levels of the bulk material. Unlike the bulk levels, the edge states are never separated from the Fermi energy by a gap. Therefore, the edge electrons can always respond to the applied external field.

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