Author
Listed:
- Hui Chen
(Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
University of Chinese Academy of Sciences
University of Chinese Academy of Sciences
Songshan Lake Materials Laboratory)
- Haitao Yang
(Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
University of Chinese Academy of Sciences
University of Chinese Academy of Sciences
Songshan Lake Materials Laboratory)
- Bin Hu
(Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
University of Chinese Academy of Sciences)
- Zhen Zhao
(Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
University of Chinese Academy of Sciences)
- Jie Yuan
(Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
University of Chinese Academy of Sciences)
- Yuqing Xing
(Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
University of Chinese Academy of Sciences)
- Guojian Qian
(Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
University of Chinese Academy of Sciences)
- Zihao Huang
(Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
University of Chinese Academy of Sciences)
- Geng Li
(Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
University of Chinese Academy of Sciences
University of Chinese Academy of Sciences)
- Yuhan Ye
(Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
University of Chinese Academy of Sciences)
- Sheng Ma
(Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
University of Chinese Academy of Sciences)
- Shunli Ni
(Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
University of Chinese Academy of Sciences)
- Hua Zhang
(Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
University of Chinese Academy of Sciences)
- Qiangwei Yin
(Renmin University of China)
- Chunsheng Gong
(Renmin University of China)
- Zhijun Tu
(Renmin University of China)
- Hechang Lei
(Renmin University of China)
- Hengxin Tan
(Weizmann Institute of Science)
- Sen Zhou
(University of Chinese Academy of Sciences
University of Chinese Academy of Sciences
Institute of Theoretical Physics, Chinese Academy of Sciences)
- Chengmin Shen
(Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
University of Chinese Academy of Sciences)
- Xiaoli Dong
(Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
University of Chinese Academy of Sciences)
- Binghai Yan
(Weizmann Institute of Science)
- Ziqiang Wang
(Boston College)
- Hong-Jun Gao
(Beijing National Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences
University of Chinese Academy of Sciences
University of Chinese Academy of Sciences
Songshan Lake Materials Laboratory)
Abstract
The transition metal kagome lattice materials host frustrated, correlated and topological quantum states of matter1–9. Recently, a new family of vanadium-based kagome metals, AV3Sb5 (A = K, Rb or Cs), with topological band structures has been discovered10,11. These layered compounds are nonmagnetic and undergo charge density wave transitions before developing superconductivity at low temperatures11–19. Here we report the observation of unconventional superconductivity and a pair density wave (PDW) in CsV3Sb5 using scanning tunnelling microscope/spectroscopy and Josephson scanning tunnelling spectroscopy. We find that CsV3Sb5 exhibits a V-shaped pairing gap Δ ~ 0.5 meV and is a strong-coupling superconductor (2Δ/kBTc ~ 5) that coexists with 4a0 unidirectional and 2a0 × 2a0 charge order. Remarkably, we discover a 3Q PDW accompanied by bidirectional 4a0/3 spatial modulations of the superconducting gap, coherence peak and gap depth in the tunnelling conductance. We term this novel quantum state a roton PDW associated with an underlying vortex–antivortex lattice that can account for the observed conductance modulations. Probing the electronic states in the vortex halo in an applied magnetic field, in strong field that suppresses superconductivity and in zero field above Tc, reveals that the PDW is a primary state responsible for an emergent pseudogap and intertwined electronic order. Our findings show striking analogies and distinctions to the phenomenology of high-Tc cuprate superconductors, and provide groundwork for understanding the microscopic origin of correlated electronic states and superconductivity in vanadium-based kagome metals.
Suggested Citation
Hui Chen & Haitao Yang & Bin Hu & Zhen Zhao & Jie Yuan & Yuqing Xing & Guojian Qian & Zihao Huang & Geng Li & Yuhan Ye & Sheng Ma & Shunli Ni & Hua Zhang & Qiangwei Yin & Chunsheng Gong & Zhijun Tu & , 2021.
"Roton pair density wave in a strong-coupling kagome superconductor,"
Nature, Nature, vol. 599(7884), pages 222-228, November.
Handle:
RePEc:nat:nature:v:599:y:2021:i:7884:d:10.1038_s41586-021-03983-5
DOI: 10.1038/s41586-021-03983-5
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