{ "id": "cond-mat/9811112", "version": "v3", "published": "1998-11-09T07:31:16.000Z", "updated": "1999-12-27T06:56:59.000Z", "title": "Insensitivity of Quantized Hall Conductance to Disorder and Interactions", "authors": [ "Tohru Koma" ], "comment": "LaTeX, 62 pages, no figures, typos corrected, some references added, discussion on the standard time-dependent vector potential added, accepted for publication in J. Stat. Phys", "categories": [ "cond-mat.mes-hall", "cond-mat.stat-mech" ], "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 non-zero 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 proved that the Hall conductance $\\sigma_{xy}$ and the diagonal conductance $\\sigma_{yy}$ satisfy $|\\sigma_{xy}+e^2\\nu/h|\\le{\\rm const.}L^{-1/12}$ and $|\\sigma_{yy}|\\le{\\rm const.}L^{-1/12}$. Here $e^2/h$ is the universal conductance with the charge $-e$ of electron and the Planck constant $h$; $\\nu$ is the filling factor of the Landau level, and $L$ is the linear dimension of the system. In the thermodymanic limit, our results show $\\sigma_{xy}=-e^2\\nu/h$ and $\\sigma_{yy}=0$. The former implies that integral and fractional filling factors $\\nu$ with a gap lead to, respectively, integral and fractional quantizations of the Hall conductance.", "revisions": [ { "version": "v3", "updated": "1999-12-27T06:56:59.000Z" } ], "analyses": { "keywords": [ "quantized hall conductance", "interactions", "insensitivity", "two-dimensional quantum hall system", "sufficiently weak electric field" ], "note": { "typesetting": "LaTeX", "pages": 62, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "1998cond.mat.11112K" } } }