{ "id": "1107.1903", "version": "v2", "published": "2011-07-10T21:39:40.000Z", "updated": "2011-09-17T11:43:03.000Z", "title": "Chiral superconductivity from repulsive interactions in doped graphene", "authors": [ "Rahul Nandkishore", "Leonid Levitov", "Andrey Chubukov" ], "journal": "Nature Physics 8, 158-163 (2012)", "doi": "10.1038/nphys2208", "categories": [ "cond-mat.mes-hall", "cond-mat.supr-con" ], "abstract": "We identify graphene as a system where chiral superconductivity can be realized. Chiral superconductivity involves a pairing gap that winds in phase around the Fermi surface, breaking time reversal symmetry. We consider a unique situation arising in graphene at a specific level of doping, where the density of states is singular, strongly enhancing the critical temperature T_c. At this doping level, the Fermi surface is nested, allowing superconductivity to emerge from repulsive electron-electron interactions. We show using a renormalization group method that superconductivity dominates over all competing orders for any choice of weak repulsive interactions. Superconductivity develops in a doubly degenerate, spin singlet channel, and a mean field calculation indicates that the superconductivity is of a chiral d+id type. We therefore predict that doped graphene can provide experimental realization of spin-singlet chiral superconductivity.", "revisions": [ { "version": "v2", "updated": "2011-09-17T11:43:03.000Z" } ], "analyses": { "keywords": [ "repulsive interactions", "doped graphene", "fermi surface", "mean field calculation", "spin singlet channel" ], "tags": [ "journal article" ], "publication": { "journal": "Nature Physics", "year": 2012, "month": "Feb", "volume": 8, "number": 2, "pages": 158 }, "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2012NatPh...8..158N" } } }