Topological superconductivity in Fibonacci quasicrystals

Топологическая сверхпроводимость в квазикристаллах Фибоначчи
Martin Leijnse, Oladunjoye A. Awoga, Annica M. Black‐Schaffer, Aksel Kobiałka, T. Domański, Patric Holmvall
2024-10-09

Fibonacci quasicrystalMajorana bound statesQC gapsshort approximantstopological superconductivity
We investigate the properties of a Fibonacci quasicrystal (QC) arrangement of a one-dimensional topological superconductor, such as a magnetic atom chain deposited on a superconducting surface. We uncover a general mutually exclusive competition between the QC properties and the topological superconducting phase with Majorana bound states (MBS): there are no MBS inside the QC gaps and the MBS never behave as QC subgap states and, likewise, no critical or winding QC subgap states exist inside the topological superconducting gaps. Surprisingly, despite this competition, we find that the QC is still highly beneficial for realizing topological superconductivity with MBS. It both leads to additional large nontrivial regions with MBS in parameter space, that are topologically trivial in crystalline systems, and increases the topological gap protecting the MBS. We also find that shorter approximants of the Fibonacci QC display the largest benefits. As a consequence, our results promote QCs, and especially their short approximants, as an appealing platform for improved experimental possibilities to realize MBS as well as generally highlight the fundamental interplay between different topologies. Published by the American Physical Society 2024
1
Despite this competition, Fibonacci QCs create additional large nontrivial regions in parameter space that host MBS but are topologically trivial in crystalline systems.
2
Fibonacci quasicrystal (QC) arrangements of 1D topological superconductors exhibit a mutually exclusive competition: Majorana bound states (MBS) do not appear inside QC gaps.
3
MBS never behave as QC subgap states, and conversely, no critical or winding QC subgap states exist inside topological superconducting gaps.
4
Shorter approximants of the Fibonacci QC provide the largest benefits for realizing and protecting MBS, making them promising for experiments.
5
The QC arrangement increases the topological gap protecting MBS compared to crystalline counterparts.

One-dimensional topological superconductor arranged in a Fibonacci quasicrystal (e.g., magnetic atom chain on a superconducting surface)

The interplay between Fibonacci quasicrystal properties and topological superconducting phase, specifically existence, protection (topological gap), and parameter-space regions of Majorana bound states and the mutual exclusion of QC subgap states and MBS

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Publication Date
2024-10-09
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Authors
Martin Leijnse
Oladunjoye A. Awoga
Annica M. Black‐Schaffer
Aksel Kobiałka
T. Domański
Patric Holmvall
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