Observation of quantum vortex core fractionalization and skyrmion formation in a superconductor

Y Yu Zheng Q Quanxin Hu (Tsung-Dao Lee Institute, School of Physics and Astronomy, and State Key Laboratory of Micro-nano Engineering Science, Shanghai Jiao Tong University, Shanghai, China.) X Xin Yu (BGI Research, Qingdao, China.) H Haijiao Ji (Tsung-Dao Lee Institute, School of Physics and Astronomy, and State Key Laboratory of Micro-nano Engineering Science, Shanghai Jiao Tong University, Shanghai, China.) I Igor Timoshuk (Department of Physics, The Royal Institute of Technology, Stockholm, Sweden.) J Julien Garaud (Institut Denis Poisson CNRS/UMR 7013, Université de Tours, Tours, France.) H Hanxiang Xu (Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, China.) Y Yongwei Li (Tsung-Dao Lee Institute, School of Physics and Astronomy, and State Key Laboratory of Micro-nano Engineering Science, Shanghai Jiao Tong University, Shanghai, China.) Y Ye Gao (Tsung-Dao Lee Institute, School of Physics and Astronomy, and State Key Laboratory of Micro-nano Engineering Science, Shanghai Jiao Tong University, Shanghai, China.) X Xingye Lu (Center for Advanced Quantum Studies, School of Physics and Astronomy, Beijing Normal University, Beijing, China.) V Vadim Grinenko (Tsung-Dao Lee Institute, School of Physics and Astronomy, and State Key Laboratory of Micro-nano Engineering Science, Shanghai Jiao Tong University, Shanghai, China.) E Egor Babaev (Department of Physics, The Royal Institute of Technology, Stockholm, Sweden.) N Noah F. Q. Yuan (Tsung-Dao Lee Institute, School of Physics and Astronomy, and State Key Laboratory of Micro-nano Engineering Science, Shanghai Jiao Tong University, Shanghai, China.) R Rui Wu (Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, China.) B Baiqing Lv (Tsung-Dao Lee Institute, School of Physics and Astronomy, and State Key Laboratory of Micro-nano Engineering Science, Shanghai Jiao Tong University, Shanghai, China.) C Chi-Ming Yim (Tsung-Dao Lee Institute, School of Physics and Astronomy, and State Key Laboratory of Micro-nano Engineering Science, Shanghai Jiao Tong University, Shanghai, China.) H Hong Ding (Tsung-Dao Lee Institute, School of Physics and Astronomy, and State Key Laboratory of Micro-nano Engineering Science, Shanghai Jiao Tong University, Shanghai, China.)

Abstract

Magnetic fields can penetrate a superconductor in the form of quantum vortices, which consist of a core singularity with circulating currents. London’s quantization implies that there is one core singularity per quantum of magnetic flux in single-component superconductors. In this study, we report signatures of quantum vortex core fractionalization on the potassium-terminated surface of a multiband superconductor, KFe 2 As 2 . The observed splitting of single integer–flux vortices into several fractional vortices results in a disparity between the numbers of flux quanta and vortex cores. These fractional vortices often arrange in chains, which calculations show are characterized by a ℂP 2 skyrmionic topological invariant; this constitutes a different type of topological defect: the chiral skyrmion. The disparate natures of integer and fractional vortices comprising skyrmions lead to distinct spectroscopic signatures.

Article Details

Journal Science
Volume / Issue Vol. 393, Issue 6806
Published July 02, 2026
Pages 80-84
ISSN 0036-8075
Publisher American Association for the Advancement of Science

Journal Info

Science

American Association for the Advancement of Science

ISSN: 0036-8075 Social Sciences

Authors (17)

Y

Yu Zheng

Q

Quanxin Hu

Tsung-Dao Lee Institute, School of Physics and Astronomy, and State Key Laboratory of Micro-nano Engineering Science, Shanghai Jiao Tong University, Shanghai, China.

X

Xin Yu

BGI Research, Qingdao, China.

H

Haijiao Ji

Tsung-Dao Lee Institute, School of Physics and Astronomy, and State Key Laboratory of Micro-nano Engineering Science, Shanghai Jiao Tong University, Shanghai, China.

I

Igor Timoshuk

Department of Physics, The Royal Institute of Technology, Stockholm, Sweden.

J

Julien Garaud

Institut Denis Poisson CNRS/UMR 7013, Université de Tours, Tours, France.

H

Hanxiang Xu

Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, China.

Y

Yongwei Li

Tsung-Dao Lee Institute, School of Physics and Astronomy, and State Key Laboratory of Micro-nano Engineering Science, Shanghai Jiao Tong University, Shanghai, China.

Y

Ye Gao

Tsung-Dao Lee Institute, School of Physics and Astronomy, and State Key Laboratory of Micro-nano Engineering Science, Shanghai Jiao Tong University, Shanghai, China.

X

Xingye Lu

Center for Advanced Quantum Studies, School of Physics and Astronomy, Beijing Normal University, Beijing, China.

V

Vadim Grinenko

Tsung-Dao Lee Institute, School of Physics and Astronomy, and State Key Laboratory of Micro-nano Engineering Science, Shanghai Jiao Tong University, Shanghai, China.

E

Egor Babaev

Department of Physics, The Royal Institute of Technology, Stockholm, Sweden.

N

Noah F. Q. Yuan

Tsung-Dao Lee Institute, School of Physics and Astronomy, and State Key Laboratory of Micro-nano Engineering Science, Shanghai Jiao Tong University, Shanghai, China.

R

Rui Wu

Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, China.

B

Baiqing Lv

Tsung-Dao Lee Institute, School of Physics and Astronomy, and State Key Laboratory of Micro-nano Engineering Science, Shanghai Jiao Tong University, Shanghai, China.

C

Chi-Ming Yim

Tsung-Dao Lee Institute, School of Physics and Astronomy, and State Key Laboratory of Micro-nano Engineering Science, Shanghai Jiao Tong University, Shanghai, China.

H

Hong Ding

Tsung-Dao Lee Institute, School of Physics and Astronomy, and State Key Laboratory of Micro-nano Engineering Science, Shanghai Jiao Tong University, Shanghai, China.