{ "id": "2012.05308", "version": "v2", "published": "2020-12-09T20:40:04.000Z", "updated": "2021-01-29T14:29:37.000Z", "title": "Tutorial: Dirac Equation Perspective on Higher-Order Topological Insulators", "authors": [ "Frank Schindler" ], "comment": "24 pages, 7 figures", "journal": "Journal of Applied Physics 128, 221102 (2020)", "doi": "10.1063/5.0035850", "categories": [ "cond-mat.mes-hall" ], "abstract": "In this tutorial, we pedagogically review recent developments in the field of non-interacting fermionic phases of matter, focussing on the low energy description of higher-order topological insulators in terms of the Dirac equation. Our aim is to give a mostly self-contained treatment. After introducing the Dirac approximation of topological crystalline band structures, we use it to derive the anomalous end and corner states of first- and higher-order topological insulators in one and two spatial dimensions. In particular, we recast the classical derivation of domain wall bound states of the Su-Schrieffer-Heeger (SSH) chain in terms of crystalline symmetry. The edge of a two-dimensional higher-order topological insulators can then be viewed as a single crystalline symmetry-protected SSH chain, whose domain wall bound states become the corner states. We never explicitly solve for the full symmetric boundary of the two-dimensional system, but instead argue by adiabatic continuity. Our approach captures all salient features of higher-order topology while remaining analytically tractable.", "revisions": [ { "version": "v2", "updated": "2021-01-29T14:29:37.000Z" } ], "analyses": { "keywords": [ "higher-order topological insulators", "dirac equation perspective", "domain wall bound states", "corner states", "single crystalline symmetry-protected ssh chain" ], "tags": [ "journal article" ], "publication": { "publisher": "AIP", "journal": "J. Appl. Phys." }, "note": { "typesetting": "TeX", "pages": 24, "language": "en", "license": "arXiv", "status": "editable" } } }