{
  "id": "cond-mat/0303253",
  "version": "v1",
  "published": "2003-03-13T16:08:37.000Z",
  "updated": "2003-03-13T16:08:37.000Z",
  "title": "Luttinger Parameter g for Metallic Carbon Nanotubes and Related Systems",
  "authors": [
    "William Que"
  ],
  "comment": "2 figures",
  "journal": "PRB66, 193405 (2002)",
  "doi": "10.1103/PhysRevB.66.193405",
  "categories": [
    "cond-mat.mes-hall",
    "cond-mat.mtrl-sci"
  ],
  "abstract": "The random phase approximation (RPA) theory is used to derive the Luttinger parameter g for metallic carbon nanotubes. The results are consistent with the Tomonaga-Luttinger models. All metallic carbon nanotubes, regardless if they are armchair tubes, zigzag tubes, or chiral tubes, should have the same Luttinger parameter g. However, a (10,10) carbon peapod should have a smaller g value than a (10,10) carbon nanotube. Changing the Fermi level by applying a gate voltage has only a second order effect on the g value. RPA theory is a valid approach to calculate plasmon energy in carbon nanotube systems, regardless if the ground state is a Luttinger liquid or Fermi liquid. (This paper was published in PRB 66, 193405 (2002). However, Eqs. (6), (9), and (19) were misprinted there.)",
  "revisions": [
    {
      "version": "v1",
      "updated": "2003-03-13T16:08:37.000Z"
    }
  ],
  "analyses": {
    "keywords": [
      "metallic carbon nanotubes",
      "luttinger parameter",
      "related systems",
      "random phase approximation",
      "carbon nanotube systems"
    ],
    "tags": [
      "journal article"
    ],
    "publication": {
      "publisher": "APS",
      "journal": "Phys. Rev. B"
    },
    "note": {
      "typesetting": "TeX",
      "pages": 0,
      "language": "en",
      "license": "arXiv",
      "status": "editable"
    }
  }
}