We construct a two-dimensional higher-order topological phase protected by a quasicrystalline eightfold rotation symmetry. Our tight-binding model describes a superconductor on the Ammann-Beenker tiling hosting localized Majorana zero modes at the corners of an octagonal sample. In order to analyze this model, we introduce Hamiltonians generated by a local rule, and use this concept to identify the bulk topological properties. We find a Z2 bulk topological invariant protecting the corner modes. Our work establishes that there exist topological phases protected by symmetries impossible in a crystal.
Beschreibung
Phys. Rev. Lett. 123, 196401 (2019) - Topological Phases without Crystalline Counterparts
%0 Journal Article
%1 PhysRevLett.123.196401
%A Varjas, Dániel
%A Lau, Alexander
%A Pöyhönen, Kim
%A Akhmerov, Anton R.
%A Pikulin, Dmitry I.
%A Fulga, Ion Cosma
%D 2019
%I American Physical Society
%J Phys. Rev. Lett.
%K a
%N 19
%P 196401
%R 10.1103/PhysRevLett.123.196401
%T Topological phases without crystalline counterparts
%U https://link.aps.org/doi/10.1103/PhysRevLett.123.196401
%V 123
%X We construct a two-dimensional higher-order topological phase protected by a quasicrystalline eightfold rotation symmetry. Our tight-binding model describes a superconductor on the Ammann-Beenker tiling hosting localized Majorana zero modes at the corners of an octagonal sample. In order to analyze this model, we introduce Hamiltonians generated by a local rule, and use this concept to identify the bulk topological properties. We find a Z2 bulk topological invariant protecting the corner modes. Our work establishes that there exist topological phases protected by symmetries impossible in a crystal.
@article{PhysRevLett.123.196401,
abstract = {We construct a two-dimensional higher-order topological phase protected by a quasicrystalline eightfold rotation symmetry. Our tight-binding model describes a superconductor on the Ammann-Beenker tiling hosting localized Majorana zero modes at the corners of an octagonal sample. In order to analyze this model, we introduce Hamiltonians generated by a local rule, and use this concept to identify the bulk topological properties. We find a Z2 bulk topological invariant protecting the corner modes. Our work establishes that there exist topological phases protected by symmetries impossible in a crystal.},
added-at = {2020-03-23T11:36:24.000+0100},
author = {Varjas, D\'aniel and Lau, Alexander and P\"oyh\"onen, Kim and Akhmerov, Anton R. and Pikulin, Dmitry I. and Fulga, Ion Cosma},
biburl = {https://www.bibsonomy.org/bibtex/2f405b9e14d209aaf16d482522951eae1/ctqmat},
day = 7,
description = {Phys. Rev. Lett. 123, 196401 (2019) - Topological Phases without Crystalline Counterparts},
doi = {10.1103/PhysRevLett.123.196401},
interhash = {1b0017c8fc727aa0509b7150489747b0},
intrahash = {f405b9e14d209aaf16d482522951eae1},
journal = {Phys. Rev. Lett.},
keywords = {a},
month = {11},
number = 19,
numpages = {6},
pages = 196401,
publisher = {American Physical Society},
timestamp = {2023-10-13T12:34:57.000+0200},
title = {Topological phases without crystalline counterparts},
url = {https://link.aps.org/doi/10.1103/PhysRevLett.123.196401},
volume = 123,
year = 2019
}