{ "id": "2008.08231", "version": "v1", "published": "2020-08-19T02:52:47.000Z", "updated": "2020-08-19T02:52:47.000Z", "title": "Spin-Orbit-Induced Topological Flat Bands in Line and Split Graphs of Bipartite Lattices", "authors": [ "Da-Shuai Ma", "Yuanfeng Xu", "Christie S. Chiu", "Nicolas Regnault", "Andrew A. Houck", "Zhida Song", "B. Andrei Bernevig" ], "categories": [ "cond-mat.mes-hall", "cond-mat.str-el" ], "abstract": "Topological flat bands, such as the band in twisted bilayer graphene, are becoming a promising platform to study topics such as correlation physics, superconductivity, and transport. In this work, we introduce a generic approach to construct two-dimensional (2D) topological quasi-flat bands from line graphs and split graphs of bipartite lattices. A line graph or split graph of a bipartite lattice exhibits a set of flat bands and a set of dispersive bands. The flat band connects to the dispersive bands through a degenerate state at some momentum. We find that, with spin-orbit coupling (SOC), the flat band becomes quasi-flat and gapped from the dispersive bands. By studying a series of specific line graphs and split graphs of bipartite lattices, we find that (i) if the flat band (without SOC) has inversion or $C_2$ symmetry and is non-degenerate, then the resulting quasi-flat band must be topologically nontrivial, and (ii) if the flat band (without SOC) is degenerate, then there exists an SOC potential such that the resulting quasi-flat band is topologically nontrivial. This generic mechanism serves as a paradigm for finding topological quasi-flat bands in 2D crystalline materials and meta-materials.", "revisions": [ { "version": "v1", "updated": "2020-08-19T02:52:47.000Z" } ], "analyses": { "keywords": [ "split graph", "bipartite lattice", "spin-orbit-induced topological flat bands", "line graph", "resulting quasi-flat band" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable" } } }