{ "id": "2007.13499", "version": "v1", "published": "2020-07-27T12:44:58.000Z", "updated": "2020-07-27T12:44:58.000Z", "title": "Non-Hermitian Bulk-Boundary Correspondence in Periodically Driven System", "authors": [ "Yang Cao", "Yang Li", "Xiaosen Yang" ], "comment": "8 pages, 4 figures", "categories": [ "cond-mat.mes-hall" ], "abstract": "Bulk-boundary correspondence, connecting the bulk topology and the edge states, is an essential principle of the topological phases. However, the bulk-boundary correspondence is broken down in general non-Hermitian systems. In this paper, we construct one-dimensional non-Hermitian Su-Schrieffer-Heeger model with periodic driving that exhibits non-Hermitian skin effects: all the eigenstates are localized at the boundary of the systems, whether the bulk states or the zero and the $\\pi$ modes. To capture the topological properties, the non-Bloch winding numbers are defined by the non-Bloch periodized evolution operators based on the generalized Brillouin zone. Furthermore, the non-Hermitian bulk-boundary correspondence is established: the non-Bloch winding numbers ($W_{0,\\pi}$) characterize the edge states with quasienergies $\\epsilon=0, \\pi$. In our non-Hermitian system, a novel phenomenon can emerge that the robust edge states can appear even when the Floquet bands are topological trivial with zero non-Bloch Chern number. We also show that the relation between the non-Bloch winding numbers and the Chern number of the Floquet bands: $C= W_{0}-W_{\\pi}$.", "revisions": [ { "version": "v1", "updated": "2020-07-27T12:44:58.000Z" } ], "analyses": { "keywords": [ "non-hermitian bulk-boundary correspondence", "periodically driven system", "non-bloch winding numbers", "edge states", "construct one-dimensional non-hermitian su-schrieffer-heeger model" ], "note": { "typesetting": "TeX", "pages": 8, "language": "en", "license": "arXiv", "status": "editable" } } }