Author
Listed:
- Ying Fu
(Shenzhen Institute for Quantum Science and Engineering, and Department of Physics, Southern University of Science and Technology)
- Miao-Ling Lin
(State Key Laboratory of Superlattices and Microstructures, Institute of Semiconductors, Chinese Academy of Sciences
Center of Materials Science and Optoelectronics Engineering & CAS Center of Excellence in Topological Quantum Computation, University of Chinese Academy of Sciences)
- Le Wang
(Shenzhen Institute for Quantum Science and Engineering, and Department of Physics, Southern University of Science and Technology)
- Qiye Liu
(Shenzhen Institute for Quantum Science and Engineering, and Department of Physics, Southern University of Science and Technology)
- Lianglong Huang
(Shenzhen Institute for Quantum Science and Engineering, and Department of Physics, Southern University of Science and Technology)
- Wenrui Jiang
(Shenzhen Institute for Quantum Science and Engineering, and Department of Physics, Southern University of Science and Technology)
- Zhanyang Hao
(Shenzhen Institute for Quantum Science and Engineering, and Department of Physics, Southern University of Science and Technology)
- Cai Liu
(Shenzhen Institute for Quantum Science and Engineering, and Department of Physics, Southern University of Science and Technology)
- Hu Zhang
(College of Physics Science and Technology, Hebei University)
- Xingqiang Shi
(College of Physics Science and Technology, Hebei University)
- Jun Zhang
(State Key Laboratory of Superlattices and Microstructures, Institute of Semiconductors, Chinese Academy of Sciences
Center of Materials Science and Optoelectronics Engineering & CAS Center of Excellence in Topological Quantum Computation, University of Chinese Academy of Sciences
Beijing Academy of Quantum Information Science)
- Junfeng Dai
(Shenzhen Institute for Quantum Science and Engineering, and Department of Physics, Southern University of Science and Technology)
- Dapeng Yu
(Shenzhen Institute for Quantum Science and Engineering, and Department of Physics, Southern University of Science and Technology)
- Fei Ye
(Shenzhen Institute for Quantum Science and Engineering, and Department of Physics, Southern University of Science and Technology
Shenzhen Key Laboratory of Advanced Quantum Functional Materials and Devices, Southern University of Science and Technology)
- Patrick A. Lee
(Department of Physics, Massachusetts Institute of Technology)
- Ping-Heng Tan
(State Key Laboratory of Superlattices and Microstructures, Institute of Semiconductors, Chinese Academy of Sciences
Center of Materials Science and Optoelectronics Engineering & CAS Center of Excellence in Topological Quantum Computation, University of Chinese Academy of Sciences
Beijing Academy of Quantum Information Science)
- Jia-Wei Mei
(Shenzhen Institute for Quantum Science and Engineering, and Department of Physics, Southern University of Science and Technology
Shenzhen Key Laboratory of Advanced Quantum Functional Materials and Devices, Southern University of Science and Technology)
Abstract
Beyond the absence of long-range magnetic orders, the most prominent feature of the elusive quantum spin liquid (QSL) state is the existence of fractionalized spin excitations, i.e., spinons. When the system orders, the spin-wave excitation appears as the bound state of the spinon-antispinon pair. Although scarcely reported, a direct comparison between similar compounds illustrates the evolution from spinon to magnon. Here, we perform the Raman scattering on single crystals of two quantum kagome antiferromagnets, of which one is the kagome QSL candidate Cu3Zn(OH)6FBr, and another is an antiferromagnetically ordered compound EuCu3(OH)6Cl3. In Cu3Zn(OH)6FBr, we identify a unique one spinon-antispinon pair component in the E2g magnetic Raman continuum, providing strong evidence for deconfined spinon excitations. In contrast, a sharp magnon peak emerges from the one-pair spinon continuum in the Eg magnetic Raman response once EuCu3(OH)6Cl3 undergoes the antiferromagnetic order transition. From the comparative Raman studies, we can regard the magnon mode as the spinon-antispinon bound state, and the spinon confinement drives the magnetic ordering.
Suggested Citation
Ying Fu & Miao-Ling Lin & Le Wang & Qiye Liu & Lianglong Huang & Wenrui Jiang & Zhanyang Hao & Cai Liu & Hu Zhang & Xingqiang Shi & Jun Zhang & Junfeng Dai & Dapeng Yu & Fei Ye & Patrick A. Lee & Ping, 2021.
"Dynamic fingerprint of fractionalized excitations in single-crystalline Cu3Zn(OH)6FBr,"
Nature Communications, Nature, vol. 12(1), pages 1-8, December.
Handle:
RePEc:nat:natcom:v:12:y:2021:i:1:d:10.1038_s41467-021-23381-9
DOI: 10.1038/s41467-021-23381-9
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