{ "id": "2204.12438", "version": "v1", "published": "2022-04-26T16:56:56.000Z", "updated": "2022-04-26T16:56:56.000Z", "title": "Brillouin Klein Bottle From Artificial Gauge Fields", "authors": [ "Z. Y. Chen", "Shengyuan A. Yang", "Y. X. Zhao" ], "journal": "Nat Commun 13, 2215 (2022)", "doi": "10.1038/s41467-022-29953-7", "categories": [ "cond-mat.mes-hall" ], "abstract": "A Brillouin zone is the unit for the momentum space of a crystal. It is topologically a torus, and distinguishing whether a set of wave functions over the Brillouin torus can be smoothly deformed to another leads to the classification of various topological states of matter. Here, we show that under $\\mathbb{Z}_2$ gauge fields, i.e., hopping amplitudes with phases $\\pm 1$, the fundamental domain of momentum space can assume the topology of a Klein bottle. This drastic change of the Brillouin zone theory is due to the projective symmetry algebra enforced by the gauge field. Remarkably, the non-orientability of the Brillouin Klein bottle corresponds to the topological classification by a $\\mathbb{Z}_2$ invariant, in contrast to the Chern number valued in $\\mathbb{Z}$ for the usual Brillouin torus. The result is a novel Klein-bottle insulator featuring topological modes at two edges related by a nonlocal twist, radically distinct from all previous topological insulators. Our prediction can be readily achieved in various artificial crystals, and the discovery opens a new direction to explore topological physics by gauge-field-modified fundamental structures of physics.", "revisions": [ { "version": "v1", "updated": "2022-04-26T16:56:56.000Z" } ], "analyses": { "keywords": [ "artificial gauge fields", "insulator featuring topological modes", "klein-bottle insulator featuring topological", "brillouin klein bottle corresponds", "brillouin zone" ], "tags": [ "journal article" ], "publication": { "publisher": "Nature" }, "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable" } } }