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Bulk localized transport states in infinite and finite quasicrystals via magnetic aperiodicity

Dean Johnstone, Matthew J. Colbrook, Anne E. B. Nielsen, Patrik Öhberg, and Callum W. Duncan
Phys. Rev. B 106, 045149 – Published 29 July 2022

Abstract

Robust edge transport can occur when charged particles in crystalline lattices interact with an applied external magnetic field. Such systems have a spectrum composed of bands of bulk states and in-gap edge states. For quasicrystalline systems, we still expect to observe the basic characteristics of bulk states and current-carrying edge states. We show that, for quasicrystals in magnetic fields, there is an additional third option—bulk localized transport (BLT) states. BLT states share the in-gap nature of the well-known edge states and can support transport, but they are fully contained within the bulk of the system, with no support along the edge. Thus, transport is possible along the edge and within distinct regions of the bulk. We consider both finite-size and infinite-size systems, using rigorous error controlled computational techniques that are not prone to finite-size effects. BLT states are preserved for infinite-size systems, in stark contrast to edge states. This allows us to observe transport in infinite-size systems, without any perturbations, defects, or boundaries being introduced. We confirm the in-gap topological nature of BLT states for finite- and infinite-size systems by computing the Bott index and local Chern marker (common topological measures). BLT states form due to magnetic aperiodicity, arising from the interplay of lengthscales between the magnetic field and the quasiperiodic lattice. BLT could have interesting applications similar to those of edge states, but now taking advantage of the larger bulk of the lattice. The infinite-size techniques introduced here, especially the calculation of topological measures, could also be widely applied to other crystalline, quasicrystalline, and disordered models.

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  • Received 6 August 2021
  • Revised 13 June 2022
  • Accepted 6 July 2022

DOI:https://doi.org/10.1103/PhysRevB.106.045149

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI. Open access publication funded by the Max Planck Society.

Published by the American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Dean Johnstone1,*,†, Matthew J. Colbrook2,3,*,‡, Anne E. B. Nielsen4,5, Patrik Öhberg1, and Callum W. Duncan6,4,§

  • 1SUPA, Institute of Photonics and Quantum Sciences, Heriot-Watt University, Edinburgh EH14 4AS, United Kingdom
  • 2Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Wilberforce Road, Cambridge CB3 0WA, United Kingdom
  • 3Centre Sciences des Données, École Normale Supérieure, 45 rue d'Ulm, 75005 Paris, France
  • 4Max-Planck-Institut für Physik komplexer Systeme, D-01187 Dresden, Germany
  • 5Department of Physics and Astronomy, Aarhus University, DK-8000 Aarhus C, Denmark
  • 6Department of Physics and SUPA, University of Strathclyde, Glasgow G4 0NG, United Kingdom

  • *These authors contributed equally to this work.
  • dj79@hw.ac.uk
  • m.colbrook@damtp.cam.ac.uk
  • §callum.duncan@strath.ac.uk

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Issue

Vol. 106, Iss. 4 — 15 July 2022

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