Berry curvature dipole induced giant mid-infrared second-harmonic generation in 2D Weyl semiconductor
Due to its inversion-broken triple helix structure and the nature of Weyl semiconductor, 2D Tellurene (2D Te) is promising to possess a strong nonlinear optical response in the infrared region, which is rarely reported in 2D materials. Here, a giant nonlinear infrared response induced by large Berry...
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Engineering::Materials Berry Curvature Dipoles Second-Harmonic Generation |
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Engineering::Materials Berry Curvature Dipoles Second-Harmonic Generation Fu, Qundong Cong, Xin Xu, Xiaodong Zhu, Song Zhao, Xiaoxu Liu, Sheng Yao, Bingqing Xu, Manzhang Deng, Ya Zhu, Chao Wang, Xiaowei Kang, Lixing Zeng, Qingsheng Lin, Miao-Ling Wang, Xingli Tang, Bijun Yang, Jianqun Dong, Zhili Liu, Fucai Xiong, Qihua Zhou, Jiadong Wang, Qijie Li, Xingji Tan, Ping-Heng Tay, Beng Kang Liu, Zheng Berry curvature dipole induced giant mid-infrared second-harmonic generation in 2D Weyl semiconductor |
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Due to its inversion-broken triple helix structure and the nature of Weyl semiconductor, 2D Tellurene (2D Te) is promising to possess a strong nonlinear optical response in the infrared region, which is rarely reported in 2D materials. Here, a giant nonlinear infrared response induced by large Berry curvature dipole (BCD) is demonstrated in the Weyl semiconductor 2D Te. Ultrahigh second-harmonic generation response is acquired from 2D Te with a large second-order nonlinear optical susceptibility (χ(2) ), which is up to 23.3 times higher than that of monolayer MoS2 in the range of 700-1500 nm. Notably, distinct from other 2D nonlinear semiconductors, χ(2) of 2D Te increases extraordinarily with increasing wavelength and reaches up to 5.58 nm V-1 at ≈2300 nm, which is the best infrared performance among the reported 2D nonlinear materials. Large χ(2) of 2D Te also enables the high-intensity sum-frequency generation with an ultralow continuous-wave (CW) pump power. Theoretical calculations reveal that the exceptional performance is attributed to the presence of large BCD located at the Weyl points of 2D Te. These results unravel a new linkage between Weyl semiconductor and strong optical nonlinear responses, rendering 2D Te a competitive candidate for highly efficient nonlinear 2D semiconductors in the infrared region. |
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School of Materials Science and Engineering |
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School of Materials Science and Engineering Fu, Qundong Cong, Xin Xu, Xiaodong Zhu, Song Zhao, Xiaoxu Liu, Sheng Yao, Bingqing Xu, Manzhang Deng, Ya Zhu, Chao Wang, Xiaowei Kang, Lixing Zeng, Qingsheng Lin, Miao-Ling Wang, Xingli Tang, Bijun Yang, Jianqun Dong, Zhili Liu, Fucai Xiong, Qihua Zhou, Jiadong Wang, Qijie Li, Xingji Tan, Ping-Heng Tay, Beng Kang Liu, Zheng |
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Article |
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Fu, Qundong Cong, Xin Xu, Xiaodong Zhu, Song Zhao, Xiaoxu Liu, Sheng Yao, Bingqing Xu, Manzhang Deng, Ya Zhu, Chao Wang, Xiaowei Kang, Lixing Zeng, Qingsheng Lin, Miao-Ling Wang, Xingli Tang, Bijun Yang, Jianqun Dong, Zhili Liu, Fucai Xiong, Qihua Zhou, Jiadong Wang, Qijie Li, Xingji Tan, Ping-Heng Tay, Beng Kang Liu, Zheng |
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Fu, Qundong |
title |
Berry curvature dipole induced giant mid-infrared second-harmonic generation in 2D Weyl semiconductor |
title_short |
Berry curvature dipole induced giant mid-infrared second-harmonic generation in 2D Weyl semiconductor |
title_full |
Berry curvature dipole induced giant mid-infrared second-harmonic generation in 2D Weyl semiconductor |
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Berry curvature dipole induced giant mid-infrared second-harmonic generation in 2D Weyl semiconductor |
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Berry curvature dipole induced giant mid-infrared second-harmonic generation in 2D Weyl semiconductor |
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berry curvature dipole induced giant mid-infrared second-harmonic generation in 2d weyl semiconductor |
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2024 |
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https://hdl.handle.net/10356/173283 |
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sg-ntu-dr.10356-1732832024-01-23T04:25:22Z Berry curvature dipole induced giant mid-infrared second-harmonic generation in 2D Weyl semiconductor Fu, Qundong Cong, Xin Xu, Xiaodong Zhu, Song Zhao, Xiaoxu Liu, Sheng Yao, Bingqing Xu, Manzhang Deng, Ya Zhu, Chao Wang, Xiaowei Kang, Lixing Zeng, Qingsheng Lin, Miao-Ling Wang, Xingli Tang, Bijun Yang, Jianqun Dong, Zhili Liu, Fucai Xiong, Qihua Zhou, Jiadong Wang, Qijie Li, Xingji Tan, Ping-Heng Tay, Beng Kang Liu, Zheng School of Materials Science and Engineering School of Electrical and Electronic Engineering School of Physical and Mathematical Sciences Institute for Functional Intelligent Materials, NUS IRL 3288 CINTRA (CNRS-NTU-THALES Research Alliances) Engineering::Materials Berry Curvature Dipoles Second-Harmonic Generation Due to its inversion-broken triple helix structure and the nature of Weyl semiconductor, 2D Tellurene (2D Te) is promising to possess a strong nonlinear optical response in the infrared region, which is rarely reported in 2D materials. Here, a giant nonlinear infrared response induced by large Berry curvature dipole (BCD) is demonstrated in the Weyl semiconductor 2D Te. Ultrahigh second-harmonic generation response is acquired from 2D Te with a large second-order nonlinear optical susceptibility (χ(2) ), which is up to 23.3 times higher than that of monolayer MoS2 in the range of 700-1500 nm. Notably, distinct from other 2D nonlinear semiconductors, χ(2) of 2D Te increases extraordinarily with increasing wavelength and reaches up to 5.58 nm V-1 at ≈2300 nm, which is the best infrared performance among the reported 2D nonlinear materials. Large χ(2) of 2D Te also enables the high-intensity sum-frequency generation with an ultralow continuous-wave (CW) pump power. Theoretical calculations reveal that the exceptional performance is attributed to the presence of large BCD located at the Weyl points of 2D Te. These results unravel a new linkage between Weyl semiconductor and strong optical nonlinear responses, rendering 2D Te a competitive candidate for highly efficient nonlinear 2D semiconductors in the infrared region. Agency for Science, Technology and Research (A*STAR) Ministry of Education (MOE) Nanyang Technological University National Research Foundation (NRF) This work was supported by the National Key Research & Development Program (2021YFE0194200), Singapore NRF-CRP21-2018-0007 and NRF-CRP22-2019-0007, Singapore Ministry of Education via AcRF Tier 3 Programme “Geometrical Quan-tum Materials” (MOE2018-T3-1-002), A*STAR under its AME IRG Grant (Award No. A2083c0052). This research/project is supported by the Ministry of Education, Singapore, under its Research Centre of Excellence award to the Institute for Functional Intelligent Materials (Project No. EDUNC-33-18-279-V12). F.L. acknowledges support from the National Key Research & Development Program (2020YFA0309200). P.T. and M.L. acknowledge support from the National Natural Science Foundation of China (Grant Nos. 12004377, 11874350, and 12204472), the CAS Key Research Program of Frontier Sciences (Grant No. ZDBS-LYSLH004) and the Strategic Priority Research Program of CAS (Grant No. XDB0460000). B.T. acknowledges funding by Singapore MOE under a Tier 2 funding (MOE2019-T2-2-075). X.Z. thanks the support from the Presidential Postdoctoral Fellowship, Nanyang Technological University, Singapore via grant 03INS000973C150. 2024-01-23T04:25:22Z 2024-01-23T04:25:22Z 2023 Journal Article Fu, Q., Cong, X., Xu, X., Zhu, S., Zhao, X., Liu, S., Yao, B., Xu, M., Deng, Y., Zhu, C., Wang, X., Kang, L., Zeng, Q., Lin, M., Wang, X., Tang, B., Yang, J., Dong, Z., Liu, F., ...Liu, Z. (2023). Berry curvature dipole induced giant mid-infrared second-harmonic generation in 2D Weyl semiconductor. Advanced Materials, 35(46), e2306330-. https://dx.doi.org/10.1002/adma.202306330 0935-9648 https://hdl.handle.net/10356/173283 10.1002/adma.202306330 37737448 2-s2.0-85174215381 46 35 e2306330 en NRF-CRP21-2018-0007 NRF-CRP22-2019-0007 MOE2018-T3-1-002 A2083c0052 EDUNC-33-18-279-V12 MOE2019-T2-2-075 03INS000973C150 Advanced Materials © 2023 Wiley-VCH GmbH. All rights reserved. |