Author
Listed:
- Yaolong Li
(Peking University)
- Yuxin Zhang
(Peking University)
- Weizhe Zhang
(Peking University)
- Xiaofang Li
(Peking University)
- Jinglin Tang
(Peking University)
- Jingying Xiao
(Peking University)
- Guanyu Zhang
(Peking University)
- Xin Liao
(Peking University)
- Pengzuo Jiang
(Peking University)
- Qinyun Liu
(Peking University)
- Yijie Luo
(Peking University)
- Zini Cao
(Peking University)
- Qinghong Lyu
(Peking University)
- Yuanbiao Tong
(Zhejiang University)
- Ruoxue Yang
(Zhejiang University)
- Hong Yang
(Peking University
Key Laboratory for Advanced Optoelectronic Integrated Chips of Jiangsu Province, Peking University Yangtze Delta Institute of Optoelectronics
Shanxi University)
- Quan Sun
(Key Laboratory for Advanced Optoelectronic Integrated Chips of Jiangsu Province, Peking University Yangtze Delta Institute of Optoelectronics)
- Yunan Gao
(Peking University
Key Laboratory for Advanced Optoelectronic Integrated Chips of Jiangsu Province, Peking University Yangtze Delta Institute of Optoelectronics
Shanxi University)
- Pan Wang
(Zhejiang University)
- Zuxin Chen
(South China Normal University)
- Wenjing Liu
(Peking University
Key Laboratory for Advanced Optoelectronic Integrated Chips of Jiangsu Province, Peking University Yangtze Delta Institute of Optoelectronics
Shanxi University)
- Shufeng Wang
(Peking University
Key Laboratory for Advanced Optoelectronic Integrated Chips of Jiangsu Province, Peking University Yangtze Delta Institute of Optoelectronics
Shanxi University)
- Guowei Lyu
(Peking University
Key Laboratory for Advanced Optoelectronic Integrated Chips of Jiangsu Province, Peking University Yangtze Delta Institute of Optoelectronics
Shanxi University)
- Xiaoyong Hu
(Peking University
Key Laboratory for Advanced Optoelectronic Integrated Chips of Jiangsu Province, Peking University Yangtze Delta Institute of Optoelectronics
Shanxi University
Hefei National Laboratory)
- Martin Aeschlimann
(Department of Physics and Research Center OPTIMAS, RPTU University Kaiserslautern-Landau)
- Qihuang Gong
(Peking University
Key Laboratory for Advanced Optoelectronic Integrated Chips of Jiangsu Province, Peking University Yangtze Delta Institute of Optoelectronics
Shanxi University
Hefei National Laboratory)
Abstract
Hyperbolic polaritons have drawn great attention in nanoscale light manipulation due to their unique properties. Currently, most studies focus on natural hyperbolic phonon materials in the mid-infrared, limiting their application in the visible to near-infrared range. Here, we present a work on broadband near-infrared hyperbolic plasmon polaritons in a van der Waals material MoOCl2 by a perturbation-free direct imaging technique of photoemission electron microscopy. In particular, the hyperbolic polariton behavior has been dynamically tailored and manipulated by wavelength, polarization, interlayer twist, and artificial structure, providing a reconfigurable platform for nanophotonic applications. Notably, the full iso-frequency contours can be reconstructed via polarization-selective excitations. Our work has contributed to hyperbolic materials in the broadband near-infrared with MoOCl2, and has revealed PEEM to be an ideal method for studying hyperbolic plasmon polaritons at the space-time limit.
Suggested Citation
Yaolong Li & Yuxin Zhang & Weizhe Zhang & Xiaofang Li & Jinglin Tang & Jingying Xiao & Guanyu Zhang & Xin Liao & Pengzuo Jiang & Qinyun Liu & Yijie Luo & Zini Cao & Qinghong Lyu & Yuanbiao Tong & Ruox, 2025.
"Broadband near-infrared hyperbolic polaritons in MoOCl2,"
Nature Communications, Nature, vol. 16(1), pages 1-8, December.
Handle:
RePEc:nat:natcom:v:16:y:2025:i:1:d:10.1038_s41467-025-61548-w
DOI: 10.1038/s41467-025-61548-w
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