Chiral light-matter interactions supported by topological edge modes at the interface of valley photonic crystals provide a robust method to implement the unidirectional spin transfer. The valley topological photonic crystals possess a pair of counterpropagating edge modes. The edge modes are robust against the sharp bend of and , which can form a resonator with whispering gallery modes. Here, we demonstrate the asymmetric emission of chiral coupling from single quantum dots in a topological resonator by tuning the coupling between a quantum emitter and a resonator mode. Under a magnetic field in Faraday configuration, the exciton state from a single quantum dot splits into two exciton spin states with opposite circularly polarized emissions due to the Zeeman effect. Two branches of the quantum dot emissions couple to a resonator mode in different degrees, resulting in an asymmetric chiral emission. Without the demanding of site-control of quantum emitters for chiral quantum optics, an extra degree of freedom to tune the chiral contrast with a topological resonator could be useful for the development of on-chip integrated photonic circuits.
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8 May 2023
Research Article|
May 09 2023
Asymmetric chiral coupling in a topological resonator
Shushu Shi
;
Shushu Shi
(Data curation, Formal analysis, Writing – original draft)
1
Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
2
CAS Center for Excellence in Topological Quantum Computation and School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100049, China
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Xin Xie;
Xin Xie
(Data curation, Formal analysis)
1
Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
2
CAS Center for Excellence in Topological Quantum Computation and School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100049, China
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Sai Yan;
Sai Yan
(Data curation, Writing – review & editing)
1
Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
2
CAS Center for Excellence in Topological Quantum Computation and School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100049, China
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Jingnan Yang;
Jingnan Yang
(Data curation, Formal analysis, Writing – original draft)
3
State Key Laboratory for Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University
, Beijing 100871, China
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Jianchen Dang;
Jianchen Dang
(Data curation, Formal analysis)
1
Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
2
CAS Center for Excellence in Topological Quantum Computation and School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100049, China
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Shan Xiao;
Shan Xiao
(Data curation, Formal analysis)
1
Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
2
CAS Center for Excellence in Topological Quantum Computation and School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100049, China
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Longlong Yang;
Longlong Yang
(Data curation, Formal analysis)
1
Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
2
CAS Center for Excellence in Topological Quantum Computation and School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100049, China
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Danjie Dai;
Danjie Dai
(Data curation, Writing – review & editing)
1
Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
2
CAS Center for Excellence in Topological Quantum Computation and School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100049, China
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Bowen Fu;
Bowen Fu
(Data curation)
3
State Key Laboratory for Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University
, Beijing 100871, China
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Yu Yuan;
Yu Yuan
(Data curation, Writing – review & editing)
1
Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
2
CAS Center for Excellence in Topological Quantum Computation and School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100049, China
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Rui Zhu
;
Rui Zhu
(Data curation)
1
Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
2
CAS Center for Excellence in Topological Quantum Computation and School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100049, China
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Xiangbin Su;
Xiangbin Su
(Resources)
4
State Key Laboratory of Superlattices and Microstructures, Institute of Semiconductors Chinese Academy of Sciences
, Beijing 100083, China
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Hanqing Liu;
Hanqing Liu
(Resources)
4
State Key Laboratory of Superlattices and Microstructures, Institute of Semiconductors Chinese Academy of Sciences
, Beijing 100083, China
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Zhanchun Zuo;
Zhanchun Zuo
(Supervision)
1
Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
2
CAS Center for Excellence in Topological Quantum Computation and School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100049, China
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Can Wang;
Can Wang
a)
(Supervision)
1
Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences
, Beijing 100190, China
2
CAS Center for Excellence in Topological Quantum Computation and School of Physical Sciences, University of Chinese Academy of Sciences
, Beijing 100049, China
5
Songshan Lake Materials Laboratory
, Dongguan, Guangdong 523808, China
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Haiqiao Ni;
Haiqiao Ni
(Resources)
4
State Key Laboratory of Superlattices and Microstructures, Institute of Semiconductors Chinese Academy of Sciences
, Beijing 100083, China
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Zhichuan Niu
;
Zhichuan Niu
(Resources)
4
State Key Laboratory of Superlattices and Microstructures, Institute of Semiconductors Chinese Academy of Sciences
, Beijing 100083, China
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Qihuang Gong;
Qihuang Gong
(Supervision)
3
State Key Laboratory for Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University
, Beijing 100871, China
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Xiulai Xu
Xiulai Xu
a)
(Conceptualization, Funding acquisition, Investigation, Supervision, Writing – review & editing)
3
State Key Laboratory for Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University
, Beijing 100871, China
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Appl. Phys. Lett. 122, 191104 (2023)
Article history
Received:
March 07 2023
Accepted:
April 26 2023
Citation
Shushu Shi, Xin Xie, Sai Yan, Jingnan Yang, Jianchen Dang, Shan Xiao, Longlong Yang, Danjie Dai, Bowen Fu, Yu Yuan, Rui Zhu, Xiangbin Su, Hanqing Liu, Zhanchun Zuo, Can Wang, Haiqiao Ni, Zhichuan Niu, Qihuang Gong, Xiulai Xu; Asymmetric chiral coupling in a topological resonator. Appl. Phys. Lett. 8 May 2023; 122 (19): 191104. https://doi.org/10.1063/5.0149671
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