{ "id": "1401.1067", "version": "v1", "published": "2014-01-06T13:22:07.000Z", "updated": "2014-01-06T13:22:07.000Z", "title": "Plasmons and their interaction with electrons in trilayer graphene", "authors": [ "P. M. Krstajić", "B. Van Duppen", "F. M. Peeters" ], "comment": "arXiv admin note: substantial text overlap with arXiv:1310.6234", "journal": "Phys. Rev. B 88, 195423 (2013)", "doi": "10.1103/PhysRevB.88.195423", "categories": [ "cond-mat.mes-hall" ], "abstract": "The interaction between electrons and plasmons in trilayer graphene is investigated within the Overhauser approach resulting in the 'plasmaron' quasi-particle. This interaction is cast into a field theoretical problem, nd its effect on the energy spectrum is calculated using improved Wigner-Brillouin perturbation theory. The plasmaron spectrum is shifted with respect to the bare electron spectrum by $\\Delta E(\\mathbf{k})\\sim 50\\div200\\,{\\rm meV}$ for ABC stacked trilayer graphene and for ABA trilayer graphene by $\\Delta E(\\mathbf{k})\\sim 30\\div150\\,{\\rm meV}$ ($\\Delta E(\\mathbf{k})\\sim 1\\div5\\,{\\rm meV}$) for the hyperbolic linear) part of the spectrum. The shift in general increases with the electron concentration $n_{e}$ and electron momentum. The dispersion of plasmarons is more pronounced in \\textit{ABC} stacked than in ABA tacked trilayer graphene, because of the different energy band structure and their different plasmon dispersion.", "revisions": [ { "version": "v1", "updated": "2014-01-06T13:22:07.000Z" } ], "analyses": { "subjects": [ "73.22.Pr", "73.20.Mf", "71.10.-w" ], "keywords": [ "interaction", "aba tacked trilayer graphene", "wigner-brillouin perturbation theory", "aba trilayer graphene", "bare electron spectrum" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Physical Review B", "year": 2013, "month": "Nov", "volume": 88, "number": 19, "pages": 195423 }, "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2013PhRvB..88s5423K" } } }