{
  "id": "0909.3111",
  "version": "v4",
  "published": "2009-09-17T19:45:15.000Z",
  "updated": "2010-01-05T20:46:02.000Z",
  "title": "Transport in line junctions of $ν=5/2$ quantum Hall liquids",
  "authors": [
    "Chenjie Wang",
    "D. E. Feldman"
  ],
  "comment": "The latest version as accepted by PRB",
  "journal": "Phys.Rev.B81:035318,2010",
  "doi": "10.1103/PhysRevB.81.035318",
  "categories": [
    "cond-mat.mes-hall",
    "cond-mat.str-el"
  ],
  "abstract": "We calculate the tunneling current through long line junctions of a $\\nu=5/2$ quantum Hall liquid and i) another $\\nu=5/2$ liquid, ii) an integer quantum Hall liquid and iii) a quantum wire. Momentum resolved tunneling provides information about the number, propagation directions and other features of the edge modes and thus helps distinguish several competing models of the 5/2 state. We investigate transport properties of two proposed Abelian states: $K=8 state and 331 state, and four possible non-Abelian states: Pfaffian, edge-reconstructed Pfaffian, and two versions of the anti-Pfaffian state. We also show that the non-equilibrated anti-Pfaffian state has a different resistance from other proposed states in the bar geometry.",
  "revisions": [
    {
      "version": "v4",
      "updated": "2010-01-05T20:46:02.000Z"
    }
  ],
  "analyses": {
    "subjects": [
      "73.43.Jn",
      "73.63.Nm",
      "73.63.Rt",
      "73.43.Cd"
    ],
    "keywords": [
      "integer quantum hall liquid",
      "anti-pfaffian state",
      "long line junctions",
      "propagation directions",
      "edge modes"
    ],
    "tags": [
      "journal article"
    ],
    "publication": {
      "publisher": "APS",
      "journal": "Physical Review B",
      "year": 2010,
      "month": "Jan",
      "volume": 81,
      "number": 3,
      "pages": "035318"
    },
    "note": {
      "typesetting": "TeX",
      "pages": 0,
      "language": "en",
      "license": "arXiv",
      "status": "editable",
      "inspire": 831787,
      "adsabs": "2010PhRvB..81c5318W"
    }
  }
}