Abstract
A two-dimensional quantum Hall system is studied for a wide class of potentials including single-body random potentials and repulsive electron–electron interactions. We assume that there exists a nonzero excitation gap above the ground state(s), and then the conductance is derived from the linear perturbation theory with a sufficiently weak electric field. Under these two assumptions, we prove that the Hall conductance σ xy and the diagonal conductance σ yy satisfy |σ xy+e 2 ν/h|≤const·L −1/2 and |σ yy|≤const·L −1/12. Here e 2/h is the universal conductance with the charge −e of the electron and the Planck constant h; ν is the filling factor of the Landau level; and L is the linear dimension of the system. In the thermodynamic limit, our results show σ xy=−e 2 ν/h and σ yy=0. The former implies that integral and fractional filling factors ν with a gap lead to, respectively, integral and fractional quantizations of the Hall conductance.
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Koma, T. Insensitivity of Quantized Hall Conductance to Disorder and Interactions. Journal of Statistical Physics 99, 383–459 (2000). https://doi.org/10.1023/A:1018657009561
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DOI: https://doi.org/10.1023/A:1018657009561