{ "id": "1803.11190", "version": "v2", "published": "2018-03-29T17:59:29.000Z", "updated": "2018-05-23T17:29:03.000Z", "title": "Unconventional superconductivity in nearly flat bands in twisted bilayer graphene", "authors": [ "Bitan Roy", "Vladimir Juricic" ], "comment": "5 pages, 2 figure: Conclusions unchanged, Version submitted to Journal on 1st of May (New RG calculation + Supplementary Materials)", "categories": [ "cond-mat.mes-hall", "cond-mat.str-el", "cond-mat.supr-con" ], "abstract": "Flat electronic bands can accommodate a plethora of interaction driven quantum phases, since kinetic energy is quenched therein and electronic interactions therefore prevail. Twisted bilayer graphene, near so-called the `magic angles', features \\emph{slow} Dirac fermions close to the charge-neutrality point (CNP) and \\emph{nearly} flat minibands around $1/4$ and $3/4$ fillings, which have also been observed in recent experiments. Starting from a continuum model of \\emph{slow} Dirac fermions, we show that with increasing chemical doping away from the CNP, a \\emph{time-reversal symmetry breaking, valley pseudo-spin-triplet, topological $p+ip$ superconductor} gradually sets in, when the system resides at the brink of an anti-ferromagnetic ordering (due to strong Hubbard repulsion), in qualitative agreement with experimental findings. The $p+ip$ paired state exhibits quantized spin and thermal Hall conductivities, polar Kerr and Faraday rotations. Our conclusion may also be operative within the minibands around $1/4$ or $3/4$ filling if they can be described in terms of slow Dirac fermions.", "revisions": [ { "version": "v2", "updated": "2018-05-23T17:29:03.000Z" } ], "analyses": { "keywords": [ "twisted bilayer graphene", "flat bands", "unconventional superconductivity", "interaction driven quantum phases", "strong hubbard repulsion" ], "note": { "typesetting": "TeX", "pages": 5, "language": "en", "license": "arXiv", "status": "editable" } } }