Proximity-induced anomalous topological superconductivity in an antiferromagnetic honeycomb-lattice

Topological superconductivity, generated in an engineered system with the proximity effect from an s-wave superconductor, usually requires the original sample to be a topological insulator. In this study, we propose a novel form of topological superconductivity in a honeycomb lattice arising from bo...

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Main Authors: Fenghua Qi, Yuanyuan Xiang, Jie Cao, Guojun Jin
Format: Article
Language:English
Published: IOP Publishing 2025-01-01
Series:New Journal of Physics
Subjects:
Online Access:https://doi.org/10.1088/1367-2630/adb779
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author Fenghua Qi
Yuanyuan Xiang
Jie Cao
Guojun Jin
author_facet Fenghua Qi
Yuanyuan Xiang
Jie Cao
Guojun Jin
author_sort Fenghua Qi
collection DOAJ
description Topological superconductivity, generated in an engineered system with the proximity effect from an s-wave superconductor, usually requires the original sample to be a topological insulator. In this study, we propose a novel form of topological superconductivity in a honeycomb lattice arising from both antiferromagnetism (AFM) and s-wave superconductivity. Eventhough the honeycomb lattice with AFM is a normal insulator, the inherent topology of such a system is nontrivial. The topology of the system is determined by the relative values of the s-wave pairing potential and antiferromagnetic order. Notably, there are no chiral edge states at the open boundary if the engineered system is uniform everywhere, whether topologically trivial or not. However, when two parts with different topologies are brought together, two chiral edge states emerge at the topological phase boundary in the middle of the material. This challenges the bulk-edge correspondence observed in conventional topological materials. These chiral edge states are protected by valley symmetry and, owing to their Majorana fermion nature, can contribute to a half-integer quantized conductance.
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spelling doaj-art-e31453f3a4ae4ad29d8907aca22bc47e2025-08-20T03:05:01ZengIOP PublishingNew Journal of Physics1367-26302025-01-0127202303710.1088/1367-2630/adb779Proximity-induced anomalous topological superconductivity in an antiferromagnetic honeycomb-latticeFenghua Qi0Yuanyuan Xiang1https://orcid.org/0000-0002-9218-1886Jie Cao2Guojun Jin3https://orcid.org/0000-0001-8184-9249School of Electronic Engineering, Nanjing Xiaozhuang University , Nanjing 211171, People’s Republic of ChinaCollege of Mechanics and Engineering Science, Hohai University , Nanjing 210098, People’s Republic of ChinaCollege of Mechanics and Engineering Science, Hohai University , Nanjing 210098, People’s Republic of ChinaNational Laboratory of Solid State Microstructures, Department of Physics, and Collaborative Innovation Center of Advanced Microstructures, Nanjing University , Nanjing 210093, People’s Republic of China; School of Physics Science and Technology, Kunming University , Kunming 650214, People’s Republic of ChinaTopological superconductivity, generated in an engineered system with the proximity effect from an s-wave superconductor, usually requires the original sample to be a topological insulator. In this study, we propose a novel form of topological superconductivity in a honeycomb lattice arising from both antiferromagnetism (AFM) and s-wave superconductivity. Eventhough the honeycomb lattice with AFM is a normal insulator, the inherent topology of such a system is nontrivial. The topology of the system is determined by the relative values of the s-wave pairing potential and antiferromagnetic order. Notably, there are no chiral edge states at the open boundary if the engineered system is uniform everywhere, whether topologically trivial or not. However, when two parts with different topologies are brought together, two chiral edge states emerge at the topological phase boundary in the middle of the material. This challenges the bulk-edge correspondence observed in conventional topological materials. These chiral edge states are protected by valley symmetry and, owing to their Majorana fermion nature, can contribute to a half-integer quantized conductance.https://doi.org/10.1088/1367-2630/adb779anomalous topological superconductivityproximityantiferromagnetic honeycomb-lattice
spellingShingle Fenghua Qi
Yuanyuan Xiang
Jie Cao
Guojun Jin
Proximity-induced anomalous topological superconductivity in an antiferromagnetic honeycomb-lattice
New Journal of Physics
anomalous topological superconductivity
proximity
antiferromagnetic honeycomb-lattice
title Proximity-induced anomalous topological superconductivity in an antiferromagnetic honeycomb-lattice
title_full Proximity-induced anomalous topological superconductivity in an antiferromagnetic honeycomb-lattice
title_fullStr Proximity-induced anomalous topological superconductivity in an antiferromagnetic honeycomb-lattice
title_full_unstemmed Proximity-induced anomalous topological superconductivity in an antiferromagnetic honeycomb-lattice
title_short Proximity-induced anomalous topological superconductivity in an antiferromagnetic honeycomb-lattice
title_sort proximity induced anomalous topological superconductivity in an antiferromagnetic honeycomb lattice
topic anomalous topological superconductivity
proximity
antiferromagnetic honeycomb-lattice
url https://doi.org/10.1088/1367-2630/adb779
work_keys_str_mv AT fenghuaqi proximityinducedanomaloustopologicalsuperconductivityinanantiferromagnetichoneycomblattice
AT yuanyuanxiang proximityinducedanomaloustopologicalsuperconductivityinanantiferromagnetichoneycomblattice
AT jiecao proximityinducedanomaloustopologicalsuperconductivityinanantiferromagnetichoneycomblattice
AT guojunjin proximityinducedanomaloustopologicalsuperconductivityinanantiferromagnetichoneycomblattice