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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Main Authors: 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
Other Authors: School of Materials Science and Engineering
Format: Article
Language:English
Published: 2024
Subjects:
Online Access:https://hdl.handle.net/10356/173283
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Institution: Nanyang Technological University
Language: English
id sg-ntu-dr.10356-173283
record_format dspace
institution Nanyang Technological University
building NTU Library
continent Asia
country Singapore
Singapore
content_provider NTU Library
collection DR-NTU
language English
topic Engineering::Materials
Berry Curvature Dipoles
Second-Harmonic Generation
spellingShingle 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
description 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.
author2 School of Materials Science and Engineering
author_facet 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
format Article
author 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
author_sort 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
title_fullStr Berry curvature dipole induced giant mid-infrared second-harmonic generation in 2D Weyl semiconductor
title_full_unstemmed Berry curvature dipole induced giant mid-infrared second-harmonic generation in 2D Weyl semiconductor
title_sort berry curvature dipole induced giant mid-infrared second-harmonic generation in 2d weyl semiconductor
publishDate 2024
url https://hdl.handle.net/10356/173283
_version_ 1789482959575711744
spelling 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.