Abstract
Whenever the Fermi level lies in a gap (or mobility gap) the bulk
Hall conductance can be expressed in a topologically invariant form
showing the quantization explicitly. The new formulation generalizes
the earlier result by Thouless, Kohmoto, Nightingale, and den Nijs
to the situation where many-body interaction and substrate disorder
are also present. When applying to the fractional quantized Hall
effect, we draw the conclusion that there must be a symmetry breaking
in the many-body ground state. The possibility of writing the fractionally
quantized Hall conductance as a topological invariant is also discussed.
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