{ "id": "1806.09418", "version": "v1", "published": "2018-06-25T12:30:49.000Z", "updated": "2018-06-25T12:30:49.000Z", "title": "Acoustic higher-order topological insulator on a Kagome lattice", "authors": [ "Haoran Xue", "Yahui Yang", "Fei Gao", "Yidong Chong", "Baile Zhang" ], "comment": "15 pages, 4 figures", "categories": [ "cond-mat.mes-hall" ], "abstract": "High-order topological insulators (TIs) are a family of recently-predicted topological phases of matter obeying an extended topological bulk-boundary correspondence principle. For example, a two-dimensional (2D) second-order TI does not exhibit gapless one-dimensional (1D) topological edge states, like a standard 2D TI, but instead has topologically-protected zero-dimensional (0D) corner states. So far, higher-order TIs have been demonstrated only in classical mechanical and electromagnetic metamaterials exhibiting quantized quadrupole polarization. Here, we experimentally realize a second-order TI in an acoustic metamaterial. This is the first experimental realization of a new type of higher-order TI, based on a breathing Kagome lattice, that has zero quadrupole polarization but nontrivial bulk topology characterized by quantized Wannier centers (WCs). Unlike previous higher-order TI realizations, the corner states depend not only on the bulk topology but also on the corner shape; we show experimentally that they exist at acute-angled corners of the Kagome lattice, but not at obtuse-angled corners. This shape dependence allows corner states to act as topologically-protected but reconfigurable local resonances.", "revisions": [ { "version": "v1", "updated": "2018-06-25T12:30:49.000Z" } ], "analyses": { "keywords": [ "acoustic higher-order topological insulator", "kagome lattice", "topological bulk-boundary correspondence principle", "exhibiting quantized quadrupole polarization", "metamaterials exhibiting quantized quadrupole" ], "note": { "typesetting": "TeX", "pages": 15, "language": "en", "license": "arXiv", "status": "editable" } } }