{ "id": "1109.0174", "version": "v2", "published": "2011-09-01T12:32:52.000Z", "updated": "2011-10-14T15:38:41.000Z", "title": "Finite-size version of the excitonic instability in graphene quantum dots", "authors": [ "Tomi Paananen", "Reinhold Egger" ], "comment": "9 pages, 10 figures, to appear in PRB", "journal": "Phys. Rev. B 84, 155456 (2011)", "doi": "10.1103/PhysRevB.84.155456", "categories": [ "cond-mat.mes-hall", "cond-mat.str-el" ], "abstract": "By a combination of Hartree-Fock simulations, exact diagonalization, and perturbative calculations, we investigate the ground-state properties of disorder-free circular quantum dots formed in a graphene monolayer. Taking the reference chemical potential at the Dirac point, we study N \\leq 15 interacting particles, where the fine structure constant {\\alpha} parametrizes the Coulomb interaction. We explore three different theoretical concepts: (i) Sucher's positive projection (\"no-pair\") approach, (ii) a more general Hamiltonian conserving both N and the number of additional electron-hole pairs, and (iii) the full quantum electrodynamics (QED) problem, where only N is conserved. We find that electron-hole pair production is important for {\\alpha} 1. This corresponds to a reconstruction of the filled Dirac sea and is a finite-size version of the bulk excitonic instability. We also address the effects of an orbital magnetic field.", "revisions": [ { "version": "v2", "updated": "2011-10-14T15:38:41.000Z" } ], "analyses": { "subjects": [ "03.65.Pm", "73.22.Pr", "71.15.Rf", "73.21.La" ], "keywords": [ "graphene quantum dots", "finite-size version", "bulk excitonic instability", "orbital magnetic field", "disorder-free circular quantum dots" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Physical Review B", "year": 2011, "month": "Oct", "volume": 84, "number": 15, "pages": 155456 }, "note": { "typesetting": "TeX", "pages": 9, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2011PhRvB..84o5456P" } } }