Robust and Clean Majorana Zero Mode in the Vortex Core of High-Temperature Superconductor (Li_{0.84}Fe_{0.16})OHFeSe

The Majorana fermion, which is its own antiparticle and obeys non-Abelian statistics, plays a critical role in topological quantum computing. It can be realized as a bound state at zero energy, called a Majorana zero mode (MZM), in the vortex core of a topological superconductor, or at the ends of a...

Full description

Bibliographic Details
Main Authors: Qin Liu, Chen Chen, Tong Zhang, Rui Peng, Ya-Jun Yan, Chen-Hao-Ping Wen, Xia Lou, Yu-Long Huang, Jin-Peng Tian, Xiao-Li Dong, Guang-Wei Wang, Wei-Cheng Bao, Qiang-Hua Wang, Zhi-Ping Yin, Zhong-Xian Zhao, Dong-Lai Feng
Format: Article
Language:English
Published: American Physical Society 2018-12-01
Series:Physical Review X
Online Access:http://doi.org/10.1103/PhysRevX.8.041056
id doaj-2df908b2cef54bc38eb39ffe4d18a09d
record_format Article
spelling doaj-2df908b2cef54bc38eb39ffe4d18a09d2020-11-24T21:34:37ZengAmerican Physical SocietyPhysical Review X2160-33082018-12-018404105610.1103/PhysRevX.8.041056Robust and Clean Majorana Zero Mode in the Vortex Core of High-Temperature Superconductor (Li_{0.84}Fe_{0.16})OHFeSeQin LiuChen ChenTong ZhangRui PengYa-Jun YanChen-Hao-Ping WenXia LouYu-Long HuangJin-Peng TianXiao-Li DongGuang-Wei WangWei-Cheng BaoQiang-Hua WangZhi-Ping YinZhong-Xian ZhaoDong-Lai FengThe Majorana fermion, which is its own antiparticle and obeys non-Abelian statistics, plays a critical role in topological quantum computing. It can be realized as a bound state at zero energy, called a Majorana zero mode (MZM), in the vortex core of a topological superconductor, or at the ends of a nanowire when both superconductivity and strong spin orbital coupling are present. A MZM can be detected as a zero-bias conductance peak (ZBCP) in tunneling spectroscopy. However, in practice, clean and robust MZMs have not been realized in the vortices of a superconductor because of contamination from impurity states or other closely packed Caroli–de Gennes-Matricon (CdGM) states, which hampers further manipulations of MZMs. Here, using scanning tunneling spectroscopy, we show that a ZBCP well separated from the other discrete CdGM states exists ubiquitously in the cores of free vortices in the defect-free regions of (Li_{0.84}Fe_{0.16})OHFeSe, which has a superconducting transition temperature of 42 K. Moreover, a Dirac-cone-type surface state is observed by angle-resolved photoemission spectroscopy, and its topological nature is confirmed by band calculations. The observed ZBCP can naturally be attributed to a MZM arising from the chiral topological surface state of a bulk superconductor. Thus, (Li_{0.84}Fe_{0.16})OHFeSe provides an ideal platform for studying MZMs and topological quantum computing.http://doi.org/10.1103/PhysRevX.8.041056
collection DOAJ
language English
format Article
sources DOAJ
author Qin Liu
Chen Chen
Tong Zhang
Rui Peng
Ya-Jun Yan
Chen-Hao-Ping Wen
Xia Lou
Yu-Long Huang
Jin-Peng Tian
Xiao-Li Dong
Guang-Wei Wang
Wei-Cheng Bao
Qiang-Hua Wang
Zhi-Ping Yin
Zhong-Xian Zhao
Dong-Lai Feng
spellingShingle Qin Liu
Chen Chen
Tong Zhang
Rui Peng
Ya-Jun Yan
Chen-Hao-Ping Wen
Xia Lou
Yu-Long Huang
Jin-Peng Tian
Xiao-Li Dong
Guang-Wei Wang
Wei-Cheng Bao
Qiang-Hua Wang
Zhi-Ping Yin
Zhong-Xian Zhao
Dong-Lai Feng
Robust and Clean Majorana Zero Mode in the Vortex Core of High-Temperature Superconductor (Li_{0.84}Fe_{0.16})OHFeSe
Physical Review X
author_facet Qin Liu
Chen Chen
Tong Zhang
Rui Peng
Ya-Jun Yan
Chen-Hao-Ping Wen
Xia Lou
Yu-Long Huang
Jin-Peng Tian
Xiao-Li Dong
Guang-Wei Wang
Wei-Cheng Bao
Qiang-Hua Wang
Zhi-Ping Yin
Zhong-Xian Zhao
Dong-Lai Feng
author_sort Qin Liu
title Robust and Clean Majorana Zero Mode in the Vortex Core of High-Temperature Superconductor (Li_{0.84}Fe_{0.16})OHFeSe
title_short Robust and Clean Majorana Zero Mode in the Vortex Core of High-Temperature Superconductor (Li_{0.84}Fe_{0.16})OHFeSe
title_full Robust and Clean Majorana Zero Mode in the Vortex Core of High-Temperature Superconductor (Li_{0.84}Fe_{0.16})OHFeSe
title_fullStr Robust and Clean Majorana Zero Mode in the Vortex Core of High-Temperature Superconductor (Li_{0.84}Fe_{0.16})OHFeSe
title_full_unstemmed Robust and Clean Majorana Zero Mode in the Vortex Core of High-Temperature Superconductor (Li_{0.84}Fe_{0.16})OHFeSe
title_sort robust and clean majorana zero mode in the vortex core of high-temperature superconductor (li_{0.84}fe_{0.16})ohfese
publisher American Physical Society
series Physical Review X
issn 2160-3308
publishDate 2018-12-01
description The Majorana fermion, which is its own antiparticle and obeys non-Abelian statistics, plays a critical role in topological quantum computing. It can be realized as a bound state at zero energy, called a Majorana zero mode (MZM), in the vortex core of a topological superconductor, or at the ends of a nanowire when both superconductivity and strong spin orbital coupling are present. A MZM can be detected as a zero-bias conductance peak (ZBCP) in tunneling spectroscopy. However, in practice, clean and robust MZMs have not been realized in the vortices of a superconductor because of contamination from impurity states or other closely packed Caroli–de Gennes-Matricon (CdGM) states, which hampers further manipulations of MZMs. Here, using scanning tunneling spectroscopy, we show that a ZBCP well separated from the other discrete CdGM states exists ubiquitously in the cores of free vortices in the defect-free regions of (Li_{0.84}Fe_{0.16})OHFeSe, which has a superconducting transition temperature of 42 K. Moreover, a Dirac-cone-type surface state is observed by angle-resolved photoemission spectroscopy, and its topological nature is confirmed by band calculations. The observed ZBCP can naturally be attributed to a MZM arising from the chiral topological surface state of a bulk superconductor. Thus, (Li_{0.84}Fe_{0.16})OHFeSe provides an ideal platform for studying MZMs and topological quantum computing.
url http://doi.org/10.1103/PhysRevX.8.041056
work_keys_str_mv AT qinliu robustandcleanmajoranazeromodeinthevortexcoreofhightemperaturesuperconductorli084fe016ohfese
AT chenchen robustandcleanmajoranazeromodeinthevortexcoreofhightemperaturesuperconductorli084fe016ohfese
AT tongzhang robustandcleanmajoranazeromodeinthevortexcoreofhightemperaturesuperconductorli084fe016ohfese
AT ruipeng robustandcleanmajoranazeromodeinthevortexcoreofhightemperaturesuperconductorli084fe016ohfese
AT yajunyan robustandcleanmajoranazeromodeinthevortexcoreofhightemperaturesuperconductorli084fe016ohfese
AT chenhaopingwen robustandcleanmajoranazeromodeinthevortexcoreofhightemperaturesuperconductorli084fe016ohfese
AT xialou robustandcleanmajoranazeromodeinthevortexcoreofhightemperaturesuperconductorli084fe016ohfese
AT yulonghuang robustandcleanmajoranazeromodeinthevortexcoreofhightemperaturesuperconductorli084fe016ohfese
AT jinpengtian robustandcleanmajoranazeromodeinthevortexcoreofhightemperaturesuperconductorli084fe016ohfese
AT xiaolidong robustandcleanmajoranazeromodeinthevortexcoreofhightemperaturesuperconductorli084fe016ohfese
AT guangweiwang robustandcleanmajoranazeromodeinthevortexcoreofhightemperaturesuperconductorli084fe016ohfese
AT weichengbao robustandcleanmajoranazeromodeinthevortexcoreofhightemperaturesuperconductorli084fe016ohfese
AT qianghuawang robustandcleanmajoranazeromodeinthevortexcoreofhightemperaturesuperconductorli084fe016ohfese
AT zhipingyin robustandcleanmajoranazeromodeinthevortexcoreofhightemperaturesuperconductorli084fe016ohfese
AT zhongxianzhao robustandcleanmajoranazeromodeinthevortexcoreofhightemperaturesuperconductorli084fe016ohfese
AT donglaifeng robustandcleanmajoranazeromodeinthevortexcoreofhightemperaturesuperconductorli084fe016ohfese
_version_ 1716695653574246400