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.

Keywords

ConductancePhysicsInvariant (physics)Quantization (signal processing)Conductance quantumQuantum Hall effectQuantum spin Hall effectCondensed matter physicsFractional quantum Hall effectQuantum mechanicsHall conductivityFermi Gamma-ray Space TelescopeHall effectTopology (electrical circuits)Electrical resistivity and conductivityElectronMathematicsQuantum wellQuantum point contactCombinatorics

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Publication Info

Year
1985
Type
article
Volume
31
Issue
6
Pages
3372-3377
Citations
1085
Access
Closed

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1085
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24
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Cite This

Qian Niu, D. J. Thouless, Yong-Shi Wu (1985). Quantized Hall conductance as a topological invariant. Physical review. B, Condensed matter , 31 (6) , 3372-3377. https://doi.org/10.1103/physrevb.31.3372

Identifiers

DOI
10.1103/physrevb.31.3372
PMID
9936224

Data Quality

Data completeness: 81%