{ "id": "cond-mat/9809228", "version": "v3", "published": "1998-09-17T06:53:13.000Z", "updated": "1999-12-27T06:36:14.000Z", "title": "Spectral Gaps of Quantum Hall Systems with Interactions", "authors": [ "Tohru Koma" ], "comment": "LaTeX, 54 pages, no figures, discussions on periodic potentials and on energy and spatial cutoffs added, typos corrected, accepted for publication in J. Stat. Phys", "categories": [ "cond-mat.mes-hall", "cond-mat.stat-mech" ], "abstract": "A two-dimensional quantum Hall system without disorder for a wide class of interactions including any two-body interaction with finite range is studied by using the Lieb-Schultz-Mattis method [{\\it Ann. Phys. (N.Y.)} {\\bf 16}: 407 (1961)]. The model is defined on an infinitely long strip with a fixed large width, and the Hilbert space is restricted to the lowest $(n_{\\rm max}+1)$ Landau levels with a large integer $n_{\\rm max}$. We proved that, for a non-integer filling $\\nu$ of the Landau levels, either (i) there is a symmetry breaking at zero temperature or (ii) there is only one infinite-volume ground state with a gapless excitation. We also proved the following two theorems: (a) If a pure infinite-volume ground state has a non-zero excitation gap for a non-integer filling $\\nu$, then a translational symmetry breaking occurs at zero temperature. (b) Suppose that there is no non-translationally invariant infinite-volume ground state. Then, if a pure infinite-volume ground state has a non-zero excitation gap, the filling factor $\\nu$ must be equal to a rational number. Here the ground state is allowed to have a periodic structure which is a consequence of the translational symmetry breaking. We also discuss the relation between our results and the quantized Hall conductance, and phenomenologically explain why odd denominators of filling fractions $\\nu$ giving the quantized Hall conductance, are favored exclusively.", "revisions": [ { "version": "v3", "updated": "1999-12-27T06:36:14.000Z" } ], "analyses": { "keywords": [ "quantum hall system", "spectral gaps", "pure infinite-volume ground state", "interaction", "non-zero excitation gap" ], "note": { "typesetting": "LaTeX", "pages": 54, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "1998cond.mat..9228K" } } }