Controlling Majorana modes by p-wave pairing in two-dimensional p+id topological superconductors

We show that corner Majorana zero modes in a two-dimensional p+id topological superconductor can be controlled by the manipulation of the parent p-wave superconducting order. Assuming that the p-wave superconducting order is in either a chiral or helical phase, we find that when a d_{x^{2}−y^{2}} wa...

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Main Authors: Morten Amundsen, Vladimir Juričić
Format: Article
Language:English
Published: American Physical Society 2022-02-01
Series:Physical Review Research
Online Access:http://doi.org/10.1103/PhysRevResearch.4.013088
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author Morten Amundsen
Vladimir Juričić
author_facet Morten Amundsen
Vladimir Juričić
author_sort Morten Amundsen
collection DOAJ
description We show that corner Majorana zero modes in a two-dimensional p+id topological superconductor can be controlled by the manipulation of the parent p-wave superconducting order. Assuming that the p-wave superconducting order is in either a chiral or helical phase, we find that when a d_{x^{2}−y^{2}} wave superconducting order is induced, the system exhibits quite different behavior depending on the nature of the parent p-wave phase. In particular, we find that while in the helical phase, a localized Majorana mode appears at each of the four corners, in the chiral phase, it is localized along only two of the four edges. We furthermore demonstrate that the Majoranas can be directly controlled by the form of the edges, as we explicitly show in the case of circular edges. We argue that the application of strain may provide additional means of fine-tuning the Majorana zero modes in the system; in particular, it can partially gap them out. Our findings may be relevant for probing the topology in two-dimensional mixed-pairing superconductors.
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spelling doaj.art-c22a5a4a8493439ca1ad7446eee3be612024-04-12T17:17:43ZengAmerican Physical SocietyPhysical Review Research2643-15642022-02-014101308810.1103/PhysRevResearch.4.013088Controlling Majorana modes by p-wave pairing in two-dimensional p+id topological superconductorsMorten AmundsenVladimir JuričićWe show that corner Majorana zero modes in a two-dimensional p+id topological superconductor can be controlled by the manipulation of the parent p-wave superconducting order. Assuming that the p-wave superconducting order is in either a chiral or helical phase, we find that when a d_{x^{2}−y^{2}} wave superconducting order is induced, the system exhibits quite different behavior depending on the nature of the parent p-wave phase. In particular, we find that while in the helical phase, a localized Majorana mode appears at each of the four corners, in the chiral phase, it is localized along only two of the four edges. We furthermore demonstrate that the Majoranas can be directly controlled by the form of the edges, as we explicitly show in the case of circular edges. We argue that the application of strain may provide additional means of fine-tuning the Majorana zero modes in the system; in particular, it can partially gap them out. Our findings may be relevant for probing the topology in two-dimensional mixed-pairing superconductors.http://doi.org/10.1103/PhysRevResearch.4.013088
spellingShingle Morten Amundsen
Vladimir Juričić
Controlling Majorana modes by p-wave pairing in two-dimensional p+id topological superconductors
Physical Review Research
title Controlling Majorana modes by p-wave pairing in two-dimensional p+id topological superconductors
title_full Controlling Majorana modes by p-wave pairing in two-dimensional p+id topological superconductors
title_fullStr Controlling Majorana modes by p-wave pairing in two-dimensional p+id topological superconductors
title_full_unstemmed Controlling Majorana modes by p-wave pairing in two-dimensional p+id topological superconductors
title_short Controlling Majorana modes by p-wave pairing in two-dimensional p+id topological superconductors
title_sort controlling majorana modes by p wave pairing in two dimensional p id topological superconductors
url http://doi.org/10.1103/PhysRevResearch.4.013088
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