{ "id": "1502.07640", "version": "v1", "published": "2015-02-26T17:21:45.000Z", "updated": "2015-02-26T17:21:45.000Z", "title": "Phase diagram of the Quantum Electrodynamics of 2D and 3D Dirac semimetals", "authors": [ "J. Gonzalez" ], "comment": "9 pages, 10 figures", "categories": [ "cond-mat.mes-hall", "cond-mat.str-el" ], "abstract": "We study the Quantum Electrodynamics of 2D and 3D Dirac semimetals by means of a self-consistent resolution of the Schwinger-Dyson equations, aiming to obtain the respective phase diagrams in terms of the relative strength of the Coulomb interaction and the number N of Dirac fermions. In this framework, 2D Dirac semimetals have just a strong-coupling instability characterized by exciton condensation (and dynamical generation of mass) that we find at a critical coupling well above previous theoretical estimates, thus explaining the absence of that instability in free-standing graphene samples. On the other hand, we show that 3D Dirac semimetals have a richer phase diagram, with a strong-coupling instability leading to dynamical mass generation up to N = 4 and a line of critical points for larger values of N characterized by the vanishing of the electron quasiparticle weight in the low-energy limit. Such a marginal Fermi liquid boundary signals the transition to a strongly renormalized electron liquid having very unstable quasiparticles, with large decay rates implying an increasing departure at strong coupling from the Fermi liquid picture.", "revisions": [ { "version": "v1", "updated": "2015-02-26T17:21:45.000Z" } ], "analyses": { "subjects": [ "71.15.Rf", "71.10.Hf", "71.30.+h", "72.80.Vp" ], "keywords": [ "3d dirac semimetals", "phase diagram", "quantum electrodynamics", "marginal fermi liquid boundary signals", "fermi liquid picture" ], "publication": { "doi": "10.1103/PhysRevB.92.125115" }, "note": { "typesetting": "TeX", "pages": 9, "language": "en", "license": "arXiv", "status": "editable", "inspire": 1346626 } } }