{ "id": "cond-mat/0011143", "version": "v1", "published": "2000-11-08T18:26:27.000Z", "updated": "2000-11-08T18:26:27.000Z", "title": "Effective Chern-Simons Theories of Pfaffian and Parafermionic Quantum Hall States, and Orbifold Conformal Field Theories", "authors": [ "Eduardo Fradkin", "Marina Huerta", "Guillermo Zemba" ], "journal": "Nucl.Phys. B601 (2001) 591-606", "doi": "10.1016/S0550-3213(01)00077-3", "categories": [ "cond-mat.mes-hall", "hep-th" ], "abstract": "We present a pure Chern-Simons formulation of families of interesting Conformal Field Theories describing edge states of non-Abelian Quantum Hall states. These theories contain two Abelian Chern-Simons fields describing the electromagnetically charged and neutral sectors of these models, respectively. The charged sector is the usual Abelian Chern-Simons theory that successfully describes Laughlin-type incompressible fluids. The neutral sector is a 2+1-dimensional theory analogous to the 1+1-dimensional orbifold conformal field theories. It is based on the gauge group O(2) which contains a ${\\bf Z}_2$ disconnected group manifold, which is the salient feature of this theory. At level q, the Abelian theory of the neutral sector gives rise to a ${\\bf Z}_{2q}$ symmetry, which is further reduced by imposing the ${\\bf Z}_2$ symmetry of charge-conjugation invariance. The remaining ${\\bf Z}_q$ symmetry of the neutral sector is the origin of the non-Abelian statistics of the (fermionic) q-Pfaffian states.", "revisions": [ { "version": "v1", "updated": "2000-11-08T18:26:27.000Z" } ], "analyses": { "keywords": [ "orbifold conformal field theories", "parafermionic quantum hall states", "effective chern-simons theories", "chern-simons theory", "neutral sector" ], "tags": [ "journal article" ], "publication": { "publisher": "Elsevier", "journal": "Nucl. Phys. B" }, "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "inspire": 536682 } } }