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Lyu X, Kallioniemi L, Cai H, An L, Duan R, Wu SJ, Tan Q, Zhang C, He R, Miao Y, Liu Z, Ling A, Zúñiga-Perez J, Gao W. Boosting classical and quantum nonlinear processes in ultrathin van der Waals materials. Nat Commun 2025; 16:4987. [PMID: 40442079 PMCID: PMC12122887 DOI: 10.1038/s41467-025-58449-3] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 06/24/2024] [Accepted: 03/24/2025] [Indexed: 06/02/2025] Open
Abstract
Understanding and controlling nonlinear processes is crucial for engineering light-matter interaction and generating non-classical light. A significant challenge in ultra-thin nonlinear materials is the marked diminution of the nonlinear conversion efficiency due to the reduced light-matter interaction length and, in many cases, the centrosymmetric crystalline structures. Here we relax these limitations and report a giant boost of classical and quantum nonlinear processes in ultrathin van der Waals materials. Specifically, with a metal-nonlinear material heterostructure we enhance classical second-harmonic generation in h-BN flakes by two orders of magnitude. Moreover, we have engineered a metal-SiO2-nonlinear material heterostructure resulting in a remarkable two orders of magnitude augmentation of the quantum spontaneous parametric down-conversion (SPDC) in NbOCl2 flakes. Notably, we demonstrate SPDC in a 16 nm-thick NbOCl2 flake integrated into the proposed structure. These findings simplify on-chip quantum state engineering and accelerate the use of van der Waals materials in nonlinear optoelectronics.
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Affiliation(s)
- Xiaodan Lyu
- Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University, Singapore, Singapore
- Majulab, International Research Laboratory IRL 3654, CNRS, Université Côte d'Azur, Sorbonne Université, National University of Singapore, Nanyang Technological University, Singapore, Singapore
| | - Leevi Kallioniemi
- Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University, Singapore, Singapore
| | - Hongbing Cai
- Department of Physics, University of Science and Technology of China, Hefei, China
| | - Liheng An
- Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University, Singapore, Singapore
| | - Ruihuan Duan
- School of Materials Science and Engineering, Nanyang Technological University, Singapore, Singapore
| | - Shuin Jian Wu
- Centre for Quantum Technologies, National University of Singapore, Singapore, Singapore
| | - Qinghai Tan
- School of Microelectronics, University of Science and Technology of China, Hefei, China
| | - Chusheng Zhang
- Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University, Singapore, Singapore
| | - Ruihua He
- School of Biological Sciences, Nanyang Technological University, Singapore, Singapore
| | - Yansong Miao
- School of Biological Sciences, Nanyang Technological University, Singapore, Singapore
| | - Zheng Liu
- School of Materials Science and Engineering, Nanyang Technological University, Singapore, Singapore
| | - Alexander Ling
- Centre for Quantum Technologies, National University of Singapore, Singapore, Singapore
- Department of Physics, National University of Singapore, Singapore, Singapore
| | - Jesus Zúñiga-Perez
- Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University, Singapore, Singapore.
- Majulab, International Research Laboratory IRL 3654, CNRS, Université Côte d'Azur, Sorbonne Université, National University of Singapore, Nanyang Technological University, Singapore, Singapore.
| | - Weibo Gao
- Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University, Singapore, Singapore.
- Majulab, International Research Laboratory IRL 3654, CNRS, Université Côte d'Azur, Sorbonne Université, National University of Singapore, Nanyang Technological University, Singapore, Singapore.
- School of Electrical and Electronic Engineering, Nanyang Technological University, Singapore, Singapore.
- Quantum Science and Engineering Centre (QSec), Nanyang Technological University, Singapore, Singapore.
- Centre for Quantum Technologies, Nanyang Technological University, Singapore, Singapore.
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2
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Xue T, Han X, Liu X, Zhao J, Yan J, Ma Y, Cai N, Wang X, Li S, Ge L, Sun Z, Huang Y, Dai Y, Wang Y. Artificially Engineered Nonlinear Circular Dichroism with Chiral Nanoscrolling of 2D Materials. NANO LETTERS 2025; 25:8399-8406. [PMID: 40354511 DOI: 10.1021/acs.nanolett.5c01780] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/14/2025]
Abstract
Nonlinear chiroptical response, particularly nonlinear circular dichroism (CD), holds significant potential for advancing nanotechnology, biophotonics, and molecular imaging. While conventional approaches rely on intrinsic chiral materials, we demonstrate a novel strategy to engineer this effect by transforming achiral two-dimensional (2D) transition-metal dichalcogenides (TMDs) into chiral nanostructures. By scrolling monolayer TMDs into geometrically chiral nanoscrolls, we achieve pronounced nonlinear CD (up to 0.8), evidenced by circular-polarization-dependent second-harmonic generation (SHG). Notably, the SHG-CD degree is tailored by controlling the nanoscrolls' scrolling axes, demonstrating, for the first time, programmable chirality-dependent nonlinear responses in TMD nanoscrolls. Furthermore, the confined electromagnetic fields within the scrolled geometry amplify the SHG intensity by up to 100-fold compared to monolayers. This chiral nanoscrolling is anticipated to enable innovative functionalities in the realm of compact nonlinear light sources and modulators, heralding a new era of advanced photonic applications.
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Affiliation(s)
- Tongtong Xue
- Advanced Research Institute of Multidisciplinary Sciences, Beijing Institute of Technology, Beijing 100081, China
| | - Xu Han
- MIIT Key Laboratory for Low-Dimensional Quantum Structure and Devices, School of Integrated Circuits and Electronics, Beijing Institute of Technology, Beijing 100081, China
| | - Xiangyu Liu
- Advanced Research Institute of Multidisciplinary Sciences, Beijing Institute of Technology, Beijing 100081, China
| | - Jinghan Zhao
- Advanced Research Institute of Multidisciplinary Sciences, Beijing Institute of Technology, Beijing 100081, China
| | - Jiahao Yan
- MIIT Key Laboratory for Low-Dimensional Quantum Structure and Devices, School of Integrated Circuits and Electronics, Beijing Institute of Technology, Beijing 100081, China
| | - Yingshan Ma
- MIIT Key Laboratory for Low-Dimensional Quantum Structure and Devices, School of Integrated Circuits and Electronics, Beijing Institute of Technology, Beijing 100081, China
| | - Ningyi Cai
- Advanced Research Institute of Multidisciplinary Sciences, Beijing Institute of Technology, Beijing 100081, China
| | - Xinyue Wang
- MIIT Key Laboratory for Low-Dimensional Quantum Structure and Devices, School of Integrated Circuits and Electronics, Beijing Institute of Technology, Beijing 100081, China
| | - Shisheng Li
- Department of Physics, Southeast University, Nanjing 210096, China
| | - Lixin Ge
- School of Physics and Electronic Engineering, Xinyang Normal University, Xinyang 464000, China
| | - Zhipei Sun
- Department of Electronics and Nanoengineering, Aalto University, Espoo 02150, Finland
| | - Yuan Huang
- Advanced Research Institute of Multidisciplinary Sciences, Beijing Institute of Technology, Beijing 100081, China
| | - Yunyun Dai
- Advanced Research Institute of Multidisciplinary Sciences, Beijing Institute of Technology, Beijing 100081, China
- MIIT Key Laboratory for Low-Dimensional Quantum Structure and Devices, School of Integrated Circuits and Electronics, Beijing Institute of Technology, Beijing 100081, China
| | - Yeliang Wang
- MIIT Key Laboratory for Low-Dimensional Quantum Structure and Devices, School of Integrated Circuits and Electronics, Beijing Institute of Technology, Beijing 100081, China
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3
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Zhu S, Chen W, Temel T, Wang F, Xu X, Duan R, Wu T, Mao X, Yan C, Yu J, Wang C, Jin Y, Cui J, Li J, Hu DJJ, Liu Z, Murray RT, Luo Y, Wang QJ. Broadband and efficient third-harmonic generation from black phosphorus-hybrid plasmonic metasurfaces in the mid-infrared. SCIENCE ADVANCES 2025; 11:eadt3772. [PMID: 40367156 PMCID: PMC12077498 DOI: 10.1126/sciadv.adt3772] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 09/25/2024] [Accepted: 04/09/2025] [Indexed: 05/16/2025]
Abstract
Black phosphorus (BP), with a mid-infrared (MIR) bandgap of 0.34 eV, presents itself as a promising material for MIR nonlinear optical applications. We report the realization of MIR third-harmonic generation (THG) in both BP and BP-hybrid plasmonic metasurfaces (BPM). BP exhibits a high third-order nonlinear susceptibility ([Formula: see text]) exceeding 10-18 m2/V2 in the MIR region with a maximum value of 1.55 × 10-17 m2/V2 at 5000 nm. The BP flake achieves a THG conversion efficiency of 1.4 × 10-5, surpassing that of other 2D materials by over one order of magnitude. To further enhance this nonlinear performance, a BPM is designed and fabricated to achieve a two-order-of-magnitude enhancement in THG, leading to a record conversion efficiency of 6.5 × 10-4, exceeding the performance of previously reported metasurfaces by more than one order of magnitude. These findings establish BP as a promising platform for next-generation MIR nonlinear optical devices.
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Affiliation(s)
- Song Zhu
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798 Singapore, Singapore
- National Key Laboratory of Microwave Photonics, Nanjing University of Aeronautics and Astronautics, Nanjing, China
| | - Wenduo Chen
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798 Singapore, Singapore
| | - Tugba Temel
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798 Singapore, Singapore
- Blackett Laboratory, Department of Physics, Imperial College London, London SW7 2BW, United Kingdom
| | - Fakun Wang
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798 Singapore, Singapore
| | - Xiaodong Xu
- School of Materials Science and Engineering, Harbin Institute of Technology, Harbin 150001, China
| | - Ruihuan Duan
- School of Materials Science and Engineering, Nanyang Technological University, 639798 Singapore, Singapore
| | - Tingting Wu
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798 Singapore, Singapore
| | - Xuan Mao
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798 Singapore, Singapore
| | - Congliao Yan
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798 Singapore, Singapore
| | - Jianbo Yu
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798 Singapore, Singapore
| | - Chongwu Wang
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798 Singapore, Singapore
| | - Yuhao Jin
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798 Singapore, Singapore
| | - Jieyuan Cui
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798 Singapore, Singapore
| | - Jinghao Li
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798 Singapore, Singapore
| | - Dora Juan Juan Hu
- Agency for Science, Technology and Research (A*STAR), Institute for Infocomm Research (I2R), 138632 Singapore, Singapore
| | - Zheng Liu
- School of Materials Science and Engineering, Nanyang Technological University, 639798 Singapore, Singapore
| | - Robert T. Murray
- Blackett Laboratory, Department of Physics, Imperial College London, London SW7 2BW, United Kingdom
| | - Yu Luo
- National Key Laboratory of Microwave Photonics, Nanjing University of Aeronautics and Astronautics, Nanjing, China
| | - Qi Jie Wang
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798 Singapore, Singapore
- School of Physical and Mathematical Sciences, Nanyang Technological University, 637371 Singapore, Singapore
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4
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Biswas R, Prosad A, A S LK, Chatterjee S, Bag U, Konkada Manattayil J, Raghunathan V. Leveraging Strong Electric Field Gradients at Anapole Resonances for Enhanced Second Harmonic Generation from Molybdenum Disulfide Disks. ADVANCED MATERIALS (DEERFIELD BEACH, FLA.) 2025; 37:e2418257. [PMID: 39995379 DOI: 10.1002/adma.202418257] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/23/2024] [Revised: 02/15/2025] [Indexed: 02/26/2025]
Abstract
Van der Waals layered materials are emerging as promising nanophotonic platforms for realizing linear and nonlinear optical devices. In particular, the high refractive indices of transition metal dichalcogenides, combined with their strong layer dependent optical properties offer interesting possibilities for designing photonic functionalities. In this study, the resonant enhancement of second harmonic generation (SHG) using molybdenum disulfide (MoS2) disks on a silicon substrate with an intermediate silicon dioxide (SiO2) layer is demonstrated. The resonant enhancement observed here is attributed to the combined interaction of the anapole scattering modes supported within the disk and Fabry-Perot (FP) modes within the multilayer stack. For a fixed MoS2 disk dimensions, an optimized SiO2 layer thickness results in constructive interference between the anapole and FP modes, thereby enhancing the fundamental field within the disk. Utilizing this resonance mechanism, SHG enhancements as high as 160 and 85-times are experimentally demonstrated when compared with unpatterned multilayer and monolayer MoS2 flakes respectively. These are the highest reported enhancement values for the widely used 2H-polytype MoS2. A significant enhancement in SHG is observed here for 2H-MoS2 despite the alternating sheet dipoles canceling the far-field emission owing to the strong electric field gradient setup within the disk at the anapole resonance.
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Affiliation(s)
- Rabindra Biswas
- Department of Electrical Communication Engineering, Indian Institute of Science, Bangalore, 560012, India
| | - Asish Prosad
- Department of Electrical Communication Engineering, Indian Institute of Science, Bangalore, 560012, India
| | - Lal Krishna A S
- Department of Electrical Communication Engineering, Indian Institute of Science, Bangalore, 560012, India
| | - Suman Chatterjee
- Department of Electrical Communication Engineering, Indian Institute of Science, Bangalore, 560012, India
| | - Urmila Bag
- Department of Electrical Communication Engineering, Indian Institute of Science, Bangalore, 560012, India
| | | | - Varun Raghunathan
- Department of Electrical Communication Engineering, Indian Institute of Science, Bangalore, 560012, India
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5
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Chen YH, Lo PY, Boschen KW, Hsu CE, Hsu YN, Holtzman LN, Peng GH, Huang CJ, Holbrook M, Wang WH, Barmak K, Hone J, Hawrylak P, Hsueh HC, Davis JA, Cheng SJ, Fuhrer MS, Chen SY. Efficient light upconversion via resonant exciton-exciton annihilation of dark excitons in few-layer transition metal dichalcogenides. Nat Commun 2025; 16:2935. [PMID: 40133279 PMCID: PMC11937314 DOI: 10.1038/s41467-025-57991-4] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 08/27/2024] [Accepted: 03/06/2025] [Indexed: 03/27/2025] Open
Abstract
Materials capable of light upconversion-transforming low-energy photons into higher-energy ones-are pivotal in advancing optoelectronics, energy solutions, and photocatalysis. However, the discovery in various materials pays little attention on few-layer transition metal dichalcogenides, primarily due to their indirect bandgaps and weaker light-matter interactions. Here, we report a pronounced light upconversion in few-layer transition metal dichalcogenides through upconversion photoluminescence spectroscopy. Our joint theory-experiment study attributes the upconversion photoluminescence to a resonant exciton-exciton annihilation involving a pair of dark excitons with opposite momenta, followed by the spontaneous emission of upconverted bright excitons, which can have a high upconversion efficiency. Additionally, the upconversion photoluminescence is generic in MoS2, MoSe2, WS2, and WSe2, showing a high tuneability from green to ultraviolet light (2.34-3.1 eV). The findings pave the way for further exploration of light upconversion regarding fundamental properties and device applications in two-dimensional semiconductors.
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Grants
- grant nos. 112 L9008 and 113 L9008 Ministry of Education (Ministry of Education, Republic of China (Taiwan))
- RGPIN-2019-05714 Gouvernement du Canada | National Research Council Canada (Conseil national de recherches Canada)
- Grant No. RGPIN-2019-05714 Gouvernement du Canada | National Research Council Canada (Conseil national de recherches Canada)
- ARC Centre of Excellence in Future Low-Energy Electronics Technologies (FLEET; CE170100039) National Science and Technology Council of Taiwan through Grant 111-2112-M-002-047 and 112-2628-M-002-008-, and the Center of Atomic Initiative for New Materials, National Taiwan University (grant nos. 112 L9008 and 113 L9008), from the Featured Areas Research Center Program within the framework of the Higher Education Sprout Project by the Ministry of Education of Taiwan.
- National Science and Technology Council of Taiwan, under the contract NSTC 112-2112-M-A49-019-MY3.
- National Science and Technology Council, Taiwan, under Grant: 110-2112-M-032-014-MY3
- University of Ottawa Research Chair in Quantum Theory of Materials, Nanostructures, and Devices
- National Science and Technology Council of Taiwan under the contract, 112-2112-M-A49-028-
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Affiliation(s)
- Yi-Hsun Chen
- School of Physics and Astronomy, Monash University, Clayton, VIC, Australia.
- Australian Research Council Centre of Excellence in Future Low-Energy Electronics Technologies (FLEET), Monash University, Clayton, VIC, Australia.
| | - Ping-Yuan Lo
- Department of Electrophysics, National Yang Ming Chiao Tung University, Hsinchu, Taiwan
| | - Kyle W Boschen
- Australian Research Council Centre of Excellence in Future Low-Energy Electronics Technologies (FLEET), Monash University, Clayton, VIC, Australia
- Optical Sciences Centre, Swinburne University of Technology, Hawthorn, VIC, Australia
| | - Chih-En Hsu
- Department of Physics, Tamkang University, New Taipei City, Taiwan
| | - Yung-Ning Hsu
- Department of Physics, Tamkang University, New Taipei City, Taiwan
| | - Luke N Holtzman
- Department of Applied Physics and Applied Mathematics, Columbia University, New York, NY, USA
| | - Guan-Hao Peng
- Department of Electrophysics, National Yang Ming Chiao Tung University, Hsinchu, Taiwan
| | - Chun-Jui Huang
- Department of Electrophysics, National Yang Ming Chiao Tung University, Hsinchu, Taiwan
| | | | - Wei-Hua Wang
- Institute of Atomic and Molecular Sciences, Academia Sinica, Taipei, Taiwan
| | - Katayun Barmak
- Department of Applied Physics and Applied Mathematics, Columbia University, New York, NY, USA
| | - James Hone
- Department of Mechanical Engineering, Columbia University, New York, NY, USA
| | - Pawel Hawrylak
- Department of Physics, University of Ottawa, Ottawa, Ontario, Canada
| | - Hung-Chung Hsueh
- Department of Physics, Tamkang University, New Taipei City, Taiwan
| | - Jeffrey A Davis
- Australian Research Council Centre of Excellence in Future Low-Energy Electronics Technologies (FLEET), Monash University, Clayton, VIC, Australia
- Optical Sciences Centre, Swinburne University of Technology, Hawthorn, VIC, Australia
| | - Shun-Jen Cheng
- Department of Electrophysics, National Yang Ming Chiao Tung University, Hsinchu, Taiwan.
| | - Michael S Fuhrer
- School of Physics and Astronomy, Monash University, Clayton, VIC, Australia
- Australian Research Council Centre of Excellence in Future Low-Energy Electronics Technologies (FLEET), Monash University, Clayton, VIC, Australia
- Monash Centre for Atomically Thin Materials, Monash University, Clayton, VIC, Australia
| | - Shao-Yu Chen
- Australian Research Council Centre of Excellence in Future Low-Energy Electronics Technologies (FLEET), Monash University, Clayton, VIC, Australia.
- Center for Condensed Matter Sciences, National Taiwan University, Taipei, Taiwan.
- Center of Atomic Initiative for New Material, National Taiwan University, Taipei, Taiwan.
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6
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Zhao Y, Chen F, Liang J, Bahramy MS, Yang M, Guang Y, Li X, Wei Z, Tang J, Zhao J, Liao M, Shen C, Wang Q, Yang R, Watanabe K, Taniguchi T, Huang Z, Shi D, Liu K, Sun Z, Feng J, Du L, Zhang G. Origin of Nonlinear Circular Photocurrent in 2D Semiconductor MoS_{2}. PHYSICAL REVIEW LETTERS 2025; 134:086201. [PMID: 40085892 DOI: 10.1103/physrevlett.134.086201] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/31/2024] [Revised: 07/18/2024] [Accepted: 01/27/2025] [Indexed: 03/16/2025]
Abstract
Nonlinear photogalvanic effects in two-dimensional materials, particularly the nonlinear circular photocurrents (NCPs) that belong to the helicity-dependent spin photocurrents, have sparked enormous research interest. Although notable progress has been witnessed, the underling origin of NCPs remains elusive. Here, we present systematic photocurrent characteristics, symmetry analysis and theoretical calculations to uncover the physical origin of NCPs in MoS_{2}, a prototypical 2D semiconductor. Our results show that the NCP responses in 2D semiconductor MoS_{2} result from the circular photon drag effect (CPDE), rather than the generally believed circular photogalvanic effect. Furthermore, we demonstrate that the NCPs are highly tunable with electrostatic doping and increase progressively with MoS_{2} thickness, evidencing the interlayer constructive nature of CPDE responses. Our Letter unravels the critical role of the previously overlooked CPDE contribution to NCPs, revolutionizing previous understanding and thus providing deep insights into further fundamental studies and technological advances in nonlinear photovoltaic and opto-spintronic devices.
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Affiliation(s)
- Yanchong Zhao
- Institute of Physics, Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Key Laboratory for Nanoscale Physics and Devices, Beijing, 100190, China
- University of Chinese Academy of Sciences, School of Physical Sciences, Beijing, 100190, China
| | - Fengyu Chen
- Peking University, School of Physics, Beijing 100871, China
| | - Jing Liang
- Peking University, School of Physics, Beijing 100871, China
- Collaborative Innovation Center of Quantum Matter, State Key Laboratory for Mesoscopic Physics, Beijing, 100871 China
| | - Mohammad Saeed Bahramy
- The University of Tokyo, Quantum-Phase Electronics Center (QPEC) and Department of Applied Physics, Tokyo 113-8656, Japan
- The University of Manchester, Department of Physics and Astronomy, School of Natural Sciences, Oxford Road, Manchester M13 9PL, United Kingdom
| | - Mingwei Yang
- Institute of Physics, Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Key Laboratory for Nanoscale Physics and Devices, Beijing, 100190, China
| | - Yao Guang
- Institute of Physics, Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Key Laboratory for Nanoscale Physics and Devices, Beijing, 100190, China
| | - Xiaomei Li
- Institute of Physics, Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Key Laboratory for Nanoscale Physics and Devices, Beijing, 100190, China
- University of Chinese Academy of Sciences, School of Physical Sciences, Beijing, 100190, China
| | - Zheng Wei
- Institute of Physics, Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Key Laboratory for Nanoscale Physics and Devices, Beijing, 100190, China
- University of Chinese Academy of Sciences, School of Physical Sciences, Beijing, 100190, China
| | - Jian Tang
- Institute of Physics, Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Key Laboratory for Nanoscale Physics and Devices, Beijing, 100190, China
- University of Chinese Academy of Sciences, School of Physical Sciences, Beijing, 100190, China
| | - Jiaojiao Zhao
- Institute of Physics, Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Key Laboratory for Nanoscale Physics and Devices, Beijing, 100190, China
- University of Chinese Academy of Sciences, School of Physical Sciences, Beijing, 100190, China
| | - Mengzhou Liao
- Institute of Physics, Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Key Laboratory for Nanoscale Physics and Devices, Beijing, 100190, China
| | - Cheng Shen
- Institute of Physics, Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Key Laboratory for Nanoscale Physics and Devices, Beijing, 100190, China
- University of Chinese Academy of Sciences, School of Physical Sciences, Beijing, 100190, China
| | - Qinqin Wang
- Institute of Physics, Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Key Laboratory for Nanoscale Physics and Devices, Beijing, 100190, China
- University of Chinese Academy of Sciences, School of Physical Sciences, Beijing, 100190, China
| | - Rong Yang
- Institute of Physics, Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Key Laboratory for Nanoscale Physics and Devices, Beijing, 100190, China
- Songshan Lake Materials Laboratory, Dongguan, Guangdong, 523808, China
| | - Kenji Watanabe
- National Institute for Materials Science, Research Center for Functional Materials, 1-1 Namiki, Tsukuba 305-0044, Japan
| | - Takashi Taniguchi
- National Institute for Materials Science, International Center for Materials Nanoarchitectonics, 1-1 Namiki, Tsukuba 305-0044, Japan
| | - Zhiheng Huang
- Institute of Physics, Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Key Laboratory for Nanoscale Physics and Devices, Beijing, 100190, China
- University of Chinese Academy of Sciences, School of Physical Sciences, Beijing, 100190, China
| | - Dongxia Shi
- Institute of Physics, Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Key Laboratory for Nanoscale Physics and Devices, Beijing, 100190, China
- University of Chinese Academy of Sciences, School of Physical Sciences, Beijing, 100190, China
| | - Kaihui Liu
- Peking University, School of Physics, Beijing 100871, China
- Collaborative Innovation Center of Quantum Matter, State Key Laboratory for Mesoscopic Physics, Beijing, 100871 China
| | - Zhipei Sun
- Aalto University, Department of Electronics and Nanoengineering, Tietotie 3, FI-02150, Finland
| | - Ji Feng
- Peking University, School of Physics, Beijing 100871, China
| | - Luojun Du
- Institute of Physics, Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Key Laboratory for Nanoscale Physics and Devices, Beijing, 100190, China
- University of Chinese Academy of Sciences, School of Physical Sciences, Beijing, 100190, China
| | - Guangyu Zhang
- Institute of Physics, Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Key Laboratory for Nanoscale Physics and Devices, Beijing, 100190, China
- University of Chinese Academy of Sciences, School of Physical Sciences, Beijing, 100190, China
- Songshan Lake Materials Laboratory, Dongguan, Guangdong, 523808, China
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7
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Li H, Zhao J, Wang Y, Liu H, Chen Q, Bao Y, Zhou M, Li Y, Sang Y, Yang F, Nie Z. Scalable Manufacturing of Low-Symmetry Plasmonic Nanospindle Arrays with Tunable Surface Lattice Resonance. ACS NANO 2025; 19:7391-7400. [PMID: 39951562 DOI: 10.1021/acsnano.4c18423] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 02/16/2025]
Abstract
Geometry-dependent plasmonic surface lattice resonances (SLRs) have garnered great interest across a range of applications, including nanolasers, sensors, photocatalysis, and nonlinear optics. However, the rational fabrication of high-quality, low-symmetry, plasmonic nanoparticle arrays over large areas remains challenging. Herein, we report a versatile strategy for the scalable fabrication of centimeter-scale plasmonic nanospindle (NS) arrays with high positional and orientational precision. Our approach combines solvent-assisted soft lithography with in situ reduction of metal precursors, enabling the cost-effective production of large-area and well-ordered NS arrays without the need of specialized equipment. The Au NS arrays exhibit superior SLRs with a ultranarrow line width of 3.9 nm and a quality factor (Q-factor) of 309. The aspect ratio and lattice geometry of the NSs can be precisely tuned by applying mechanical strain to the stretchable elastomeric template, thus, allowing us to customize the SLR performance across the near-infrared spectrum. This technique enables the precise engineering of anisotropic nanoparticle arrays in a standard chemistry laboratory, opening new possibilities for advanced plasmonic devices.
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Affiliation(s)
- Hongyan Li
- State Key Laboratory of Molecular Engineering of Polymers, Department of Macromolecular Science, Fudan University, 200433 Shanghai, China
| | - Jingyi Zhao
- Department of Physics, Key Laboratory of Micro- and Nano-Photonic Structures (Ministry of Education), and State Key Laboratory of Surface Physics, Fudan University, 200433 Shanghai, China
| | - Yazi Wang
- State Key Laboratory of Molecular Engineering of Polymers, Department of Macromolecular Science, Fudan University, 200433 Shanghai, China
| | - Haitao Liu
- School of Physical Science and Technology, Tiangong University, 300387 Tianjin, China
| | - Qianyun Chen
- State Key Laboratory of Molecular Engineering of Polymers, Department of Macromolecular Science, Fudan University, 200433 Shanghai, China
| | - Yilin Bao
- State Key Laboratory of Molecular Engineering of Polymers, Department of Macromolecular Science, Fudan University, 200433 Shanghai, China
| | - Miaoen Zhou
- State Key Laboratory of Molecular Engineering of Polymers, Department of Macromolecular Science, Fudan University, 200433 Shanghai, China
| | - Yue Li
- School of Physical Science and Technology, Tiangong University, 300387 Tianjin, China
| | - Yutao Sang
- State Key Laboratory of Molecular Engineering of Polymers, Department of Macromolecular Science, Fudan University, 200433 Shanghai, China
| | - Fan Yang
- School of Physical Science and Technology, Tiangong University, 300387 Tianjin, China
| | - Zhihong Nie
- State Key Laboratory of Molecular Engineering of Polymers, Department of Macromolecular Science, Fudan University, 200433 Shanghai, China
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8
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Li Y, Xin J, Guo Y, Li Z, Zhang X. Ferroelectricity and Nonlinear Optical Responses in Two-Dimensional Distorted MX2Y ( M = Cu, Ag, Au; X = Chalcogens; Y = Halogen) Monolayers. ACS APPLIED MATERIALS & INTERFACES 2025; 17:6755-6762. [PMID: 39832882 DOI: 10.1021/acsami.4c19036] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 01/22/2025]
Abstract
Two-dimensional (2D) materials with spontaneous polarization can exhibit large second-order nonlinear optical (NLO) effects. Here, we present a series of stable distorted MX2Y monolayers by using first-principles calculations and lattice vibration analysis. The structural distortion leads to a lower polar symmetry, giving rise to intrinsic ferroelectricity with a Curie point up to room temperature. We show that the bulk photovoltaic effect (BPVE) in polar MX2Y monolayers has an enhanced shift current, an order of magnitude larger than that in the undistorted nonpolar counterparts. Meanwhile, the second harmonic generation (SHG) susceptibility reaches up to the order of 106 pm2/V, superior to that of 2D conventional materials such as MoS2, h-BN, and GeS. Our study advances the research in 2D ferroelectric materials and would stimulate more efforts in developing optoelectronic devices based on NLO effects.
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Affiliation(s)
- Yanlin Li
- Department of Physics, School of Physical Science and Engineering, Beijing Jiaotong University, Beijing 100044, China
| | - Jiaqi Xin
- Department of Physics, School of Physical Science and Engineering, Beijing Jiaotong University, Beijing 100044, China
| | - Yaguang Guo
- Department of Physics, School of Physical Science and Engineering, Beijing Jiaotong University, Beijing 100044, China
| | - Zhengyong Li
- Department of Physics, School of Physical Science and Engineering, Beijing Jiaotong University, Beijing 100044, China
| | - Xinghua Zhang
- Department of Physics, School of Physical Science and Engineering, Beijing Jiaotong University, Beijing 100044, China
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9
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Wei J, Hu F, Lv C, Bian L, Quan X, Ouyang Q. Fabrication of Dual-Functional MXene@NiCo 2S 4 Composites with Enhanced Nonlinear Optical and Electrochemical Properties. SMALL (WEINHEIM AN DER BERGSTRASSE, GERMANY) 2025:e2411146. [PMID: 39871764 DOI: 10.1002/smll.202411146] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/21/2024] [Revised: 01/21/2025] [Indexed: 01/29/2025]
Abstract
The design and synthesis of multifunctional nanomaterials have attracted considerable attention for expanding the range of practical applications. Herein, a metal-organic framework (MOFs)-derived NiCo2S4 attached to MXene is rationally designed and constructed for an optical limiter and supercapacitor. The MOF-derived NiCo2S4 enhances the tendency of hydroxyl groups on the MXene surface to attract metal ions, resulting in the formation of sulfur vacancies. Moreover, MXene offers a high specific surface area to facilitate the rapid complexation of charge carriers. The resultant MXene@NiCo2S4 (MX@NCS) exhibits markedly enhanced nonlinear optical (NLO) and electrochemical properties through synergistic interactions between the components. The NLO properties can be further optimized by adjusting the amount of MX@NCS powder dispersed in methyl methacrylate (MX@NCS)2-6/PMMA) by using the Z-scan technique. Specifically, the (MX@NCS)4/PMMA exhibits the strongest reverse saturable absorption (RSA) and self-defocusing effects at 100 µJ with β = 3.87 × 102 cm·GW-1 and γ = -5.94 × 10-4 cm2·GW-1. Concurrently, the constructed supercapacitor shows a superior energy density of 51.21 Wh·kg-1 at a power density of 863.65 W·kg-1. Notably, the present study indicates a novel strategy to explore the application of materials in the development of efficient optical limiter and supercapacitor technologies.
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Affiliation(s)
- Jinhe Wei
- Key Laboratory of Photonic Materials and Devices Physics for Oceanic Applications, Ministry of Industry and Information Technology of China, College of Physics and Optoelectronic Engineering, Harbin Engineering University, Harbin, 150001, China
- Key Laboratory of In-Fiber Integrated Optics of Ministry of Education, College of Physics and Optoelectronic Engineering, Harbin Engineering University, Harbin, 150001, China
| | - Fei Hu
- Key Laboratory of Photonic Materials and Devices Physics for Oceanic Applications, Ministry of Industry and Information Technology of China, College of Physics and Optoelectronic Engineering, Harbin Engineering University, Harbin, 150001, China
- Key Laboratory of In-Fiber Integrated Optics of Ministry of Education, College of Physics and Optoelectronic Engineering, Harbin Engineering University, Harbin, 150001, China
| | - Chenglong Lv
- Key Laboratory of Photonic Materials and Devices Physics for Oceanic Applications, Ministry of Industry and Information Technology of China, College of Physics and Optoelectronic Engineering, Harbin Engineering University, Harbin, 150001, China
- Key Laboratory of In-Fiber Integrated Optics of Ministry of Education, College of Physics and Optoelectronic Engineering, Harbin Engineering University, Harbin, 150001, China
| | - Limin Bian
- Key Laboratory of Photonic Materials and Devices Physics for Oceanic Applications, Ministry of Industry and Information Technology of China, College of Physics and Optoelectronic Engineering, Harbin Engineering University, Harbin, 150001, China
- Key Laboratory of In-Fiber Integrated Optics of Ministry of Education, College of Physics and Optoelectronic Engineering, Harbin Engineering University, Harbin, 150001, China
| | - Xinyu Quan
- Key Laboratory of Photonic Materials and Devices Physics for Oceanic Applications, Ministry of Industry and Information Technology of China, College of Physics and Optoelectronic Engineering, Harbin Engineering University, Harbin, 150001, China
- Key Laboratory of In-Fiber Integrated Optics of Ministry of Education, College of Physics and Optoelectronic Engineering, Harbin Engineering University, Harbin, 150001, China
| | - Qiuyun Ouyang
- Key Laboratory of Photonic Materials and Devices Physics for Oceanic Applications, Ministry of Industry and Information Technology of China, College of Physics and Optoelectronic Engineering, Harbin Engineering University, Harbin, 150001, China
- Key Laboratory of In-Fiber Integrated Optics of Ministry of Education, College of Physics and Optoelectronic Engineering, Harbin Engineering University, Harbin, 150001, China
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10
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Liang H, Gu T, Lou Y, Yang C, Ma C, Qi J, Bettiol AA, Wang X. Tunable polarization entangled photon-pair source in rhombohedral boron nitride. SCIENCE ADVANCES 2025; 11:eadt3710. [PMID: 39841823 PMCID: PMC11753379 DOI: 10.1126/sciadv.adt3710] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/24/2024] [Accepted: 12/19/2024] [Indexed: 01/24/2025]
Abstract
Entangled photon-pair sources are pivotal in various quantum applications. Miniaturizing the quantum devices to meet the requirement in limited space applications drives the search for ultracompact entangled photon-pair sources. The rise of two-dimensional (2D) semiconductors has been demonstrated as ultracompact entangled photon-pair sources. However, the photon-pair generation rate and purity are relatively low, and the strong photoluminescence in 2D semiconductors also makes the operational wavelength range limited. Here, we use the spontaneous parametric down conversion (SPDC) of rhombohedral boron nitride (rBN) as a polarization entangled photon-pair source. We have achieved a generation rate of more than 120 hertz (a record-high SPDC coincidence rate with 2D materials) and a high-purity photon-pair generation with a coincidence-to-accidental ratio of above 200. Tunable Bell state generation is also demonstrated by simply rotating the pump polarization, with a fidelity up to 0.93. Our results suggest rBN as an ideal candidate for on-chip integrated quantum devices.
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Affiliation(s)
- Haidong Liang
- Centre for Ion Beam Applications (CIBA), Department of Physics, National University of Singapore, Singapore 117542, Singapore
| | - Tian Gu
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing 100871, China
| | - Yanchao Lou
- National Laboratory of Solid State Microstructures and School of Physics, Nanjing University, Nanjing 210093, China
| | - Chengyuan Yang
- Centre for Ion Beam Applications (CIBA), Department of Physics, National University of Singapore, Singapore 117542, Singapore
| | - Chaojie Ma
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing 100871, China
- Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
| | - Jiajie Qi
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing 100871, China
| | - Andrew A. Bettiol
- Centre for Ion Beam Applications (CIBA), Department of Physics, National University of Singapore, Singapore 117542, Singapore
| | - Xilin Wang
- National Laboratory of Solid State Microstructures and School of Physics, Nanjing University, Nanjing 210093, China
- Hefei National Laboratory, Hefei 230088, China
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11
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Tan Z, Dong J, Liu Y, Luo Q, Li Z, Yun T, Jiang T, Cheng X, Huang D. Nonlinear optics of graphitic carbon allotropes: from 0D to 3D. NANOSCALE 2025; 17:1171-1212. [PMID: 39630118 DOI: 10.1039/d4nr03467h] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 12/07/2024]
Abstract
The dimensionality of materials fundamentally influences their electronic and optical properties, presenting a complex interplay with nonlinear optical (NLO) characteristics that remains largely unexplored. In this review, we focus on the influence of dimensionality on the NLO properties of graphitic allotropes, ranging from 0D fullerenes, 1D carbon nanotubes, and 2D graphene, to 3D graphite, all of which share a consistent sp2 hybridized chemical bonding structure. We examine the distinct physical and NLO properties across these dimensions, underscoring the profound impact of dimensionality. Notably, dimension-specific physical phenomena, such as Luttinger liquid in 1D and Landau quantization in 2D, play a significant role in shaping NLO phenomena. Finally, we explore the promising potential of NLO properties in systems with mixed dimensionalities, setting the stage for future breakthroughs and innovative applications.
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Affiliation(s)
- Zhengyang Tan
- MOE Key Laboratory of Advanced Micro-Structured Materials, Shanghai Frontiers Science Center of Digital Optics, Institute of Precision Optical Engineering, and School of Physics Science and Engineering, Tongji University, Shanghai, 200092, China.
| | - Jiakai Dong
- MOE Key Laboratory of Advanced Micro-Structured Materials, Shanghai Frontiers Science Center of Digital Optics, Institute of Precision Optical Engineering, and School of Physics Science and Engineering, Tongji University, Shanghai, 200092, China.
| | - Yang Liu
- MOE Key Laboratory of Advanced Micro-Structured Materials, Shanghai Frontiers Science Center of Digital Optics, Institute of Precision Optical Engineering, and School of Physics Science and Engineering, Tongji University, Shanghai, 200092, China.
| | - Qi Luo
- MOE Key Laboratory of Advanced Micro-Structured Materials, Shanghai Frontiers Science Center of Digital Optics, Institute of Precision Optical Engineering, and School of Physics Science and Engineering, Tongji University, Shanghai, 200092, China.
| | - Zhengyang Li
- MOE Key Laboratory of Advanced Micro-Structured Materials, Shanghai Frontiers Science Center of Digital Optics, Institute of Precision Optical Engineering, and School of Physics Science and Engineering, Tongji University, Shanghai, 200092, China.
| | - Tiantian Yun
- MOE Key Laboratory of Advanced Micro-Structured Materials, Shanghai Frontiers Science Center of Digital Optics, Institute of Precision Optical Engineering, and School of Physics Science and Engineering, Tongji University, Shanghai, 200092, China.
| | - Tao Jiang
- MOE Key Laboratory of Advanced Micro-Structured Materials, Shanghai Frontiers Science Center of Digital Optics, Institute of Precision Optical Engineering, and School of Physics Science and Engineering, Tongji University, Shanghai, 200092, China.
- Shanghai Institute of Intelligent Science and Technology, Tongji University, Shanghai, 200092, China
| | - Xinbin Cheng
- MOE Key Laboratory of Advanced Micro-Structured Materials, Shanghai Frontiers Science Center of Digital Optics, Institute of Precision Optical Engineering, and School of Physics Science and Engineering, Tongji University, Shanghai, 200092, China.
- Shanghai Institute of Intelligent Science and Technology, Tongji University, Shanghai, 200092, China
| | - Di Huang
- MOE Key Laboratory of Advanced Micro-Structured Materials, Shanghai Frontiers Science Center of Digital Optics, Institute of Precision Optical Engineering, and School of Physics Science and Engineering, Tongji University, Shanghai, 200092, China.
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12
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Das S, Uddin MG, Li D, Wang Y, Dai Y, Toivonen J, Hong H, Liu K, Sun Z. Nanoscale thickness Octave-spanning coherent supercontinuum light generation. LIGHT, SCIENCE & APPLICATIONS 2025; 14:41. [PMID: 39779663 PMCID: PMC11711750 DOI: 10.1038/s41377-024-01660-6] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 05/07/2024] [Revised: 10/01/2024] [Accepted: 10/13/2024] [Indexed: 01/11/2025]
Abstract
Coherent broadband light generation has attracted massive attention due to its numerous applications ranging from metrology, sensing, and imaging to communication. In general, spectral broadening is realized via third-order and higher-order nonlinear optical processes (e.g., self-phase modulation, Raman transition, four-wave mixing, multiwave mixing), which are typically weak and thus require a long interaction length and the phase matching condition to enhance the efficient nonlinear light-matter interaction for broad-spectrum generation. Here, for the first time, we report octave-spanning coherent light generation at the nanometer scale enabled by a phase-matching-free frequency down-conversion process. Up to octave-spanning coherent light generation with a -40dB spectral width covering from ~565 to 1906 nm is demonstrated in discreate manner via difference-frequency generation, a second-order nonlinear process in gallium selenide and niobium oxide diiodide crystals at the 100-nanometer scale. Compared with conventional coherent broadband light sources based on bulk materials, our demonstration is ~5 orders of magnitude thinner and requires ~3 orders of magnitude lower excitation power. Our results open a new way to possibly create compact, versatile and integrated ultra-broadband light sources.
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Affiliation(s)
- Susobhan Das
- Department of Electronics and Nanoengineering, Aalto University, Espoo, Finland.
- QTF Centre of Excellence, Department of Applied Physics, Aalto University, Aalto, Finland.
| | - Md Gius Uddin
- Department of Electronics and Nanoengineering, Aalto University, Espoo, Finland
- QTF Centre of Excellence, Department of Applied Physics, Aalto University, Aalto, Finland
| | - Diao Li
- Department of Electronics and Nanoengineering, Aalto University, Espoo, Finland
| | - Yadong Wang
- Department of Electronics and Nanoengineering, Aalto University, Espoo, Finland
| | - Yunyun Dai
- Department of Electronics and Nanoengineering, Aalto University, Espoo, Finland
| | - Juha Toivonen
- Department of Engineering and Natural Sciences, Tampere University, Tampere, Finland
| | - Hao Hong
- State Key Laboratory for Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, Beijing, China
| | - Kaihui Liu
- State Key Laboratory for Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, Beijing, China
| | - Zhipei Sun
- Department of Electronics and Nanoengineering, Aalto University, Espoo, Finland.
- QTF Centre of Excellence, Department of Applied Physics, Aalto University, Aalto, Finland.
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13
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Morey MM, Bahadur R, Li Z, Dharmarajan NP, Fawaz M, Bandyopadhyay A, Chahal S, Ansah S, Singh Raman RK, Terrones M, Kumar P, Vinu A. Experimental Realization of Fluoroborophene. SMALL (WEINHEIM AN DER BERGSTRASSE, GERMANY) 2025; 21:e2407763. [PMID: 39479754 DOI: 10.1002/smll.202407763] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/30/2024] [Revised: 10/11/2024] [Indexed: 01/11/2025]
Abstract
Borophene, an anisotropic metallic Dirac material exhibits superlative physical and chemical properties. While the lack of bandgap restricts its electronic chip applications, insufficient charge carrier density and electrochemical/catalytically active sites, restricts its energy storage and catalysis applications. Fluorination of borophene can induce bandgap and yield local electron injection within its crystallographic lattice. Herein, a facile synthesis of fluoroborophene with tunable fluorine content through potassium fluoride-assisted solvothermal-sonochemical combinatorial approach is reported. Fluoroborophene monolayers with lateral dimension 50 nm-5 µm are synthesized having controlled fluorine content (12-35%). Fluoroborophene exhibits inter-twinned crystallographic structure, with fluorination-tunable visible-range bandgap ≈1.5-2.5 eV, and density functional theory calculations also corroborate it. Fluoroborophene is explored for electrocatalytic oxygen evolution reaction in an alkaline medium and bestow a good stability. Tunable bandgap, electrophilicity and molecular anchoring capability of fluoroborophene will open opportunities for novel electronic/optoelectronic/spintronic chips, energy storage devices, and in numerous catalytic applications.
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Affiliation(s)
- Mukul M Morey
- Global Innovative Centre for Advanced Nanomaterials (GICAN), School of Engineering, College of Engineering, Science and Environment, The University of Newcastle, Callaghan, NSW, 2308, Australia
| | - Rohan Bahadur
- Global Innovative Centre for Advanced Nanomaterials (GICAN), School of Engineering, College of Engineering, Science and Environment, The University of Newcastle, Callaghan, NSW, 2308, Australia
| | - Zhixuan Li
- Global Innovative Centre for Advanced Nanomaterials (GICAN), School of Engineering, College of Engineering, Science and Environment, The University of Newcastle, Callaghan, NSW, 2308, Australia
| | - Nithinraj P Dharmarajan
- Global Innovative Centre for Advanced Nanomaterials (GICAN), School of Engineering, College of Engineering, Science and Environment, The University of Newcastle, Callaghan, NSW, 2308, Australia
| | - Mohammed Fawaz
- Global Innovative Centre for Advanced Nanomaterials (GICAN), School of Engineering, College of Engineering, Science and Environment, The University of Newcastle, Callaghan, NSW, 2308, Australia
| | - Arkamita Bandyopadhyay
- Institut für Physik, Theoretische Physik, Martin-Luther-Universität Halle-Wittenber, 06120, Halle, Germany
| | - Sumit Chahal
- Department of Physics, Indian Institute of Technology Hyderabad, Sangareddy, Kandi, Telangana, 502285, India
| | - Solomon Ansah
- Department of Mechanical & Aerospace Engineering, Monash University, Clayton, Victoria, 3800, Australia
| | - R K Singh Raman
- Department of Mechanical & Aerospace Engineering, Monash University, Clayton, Victoria, 3800, Australia
- Department of Chemical & Biological Engineering, Monash University, Clayton, Victoria, 3800, Australia
| | - Mauricio Terrones
- Center for 2-Dimensional and Layered Materials, The Pennsylvania State University, University Park, PA, 16802, USA
| | - Prashant Kumar
- Global Innovative Centre for Advanced Nanomaterials (GICAN), School of Engineering, College of Engineering, Science and Environment, The University of Newcastle, Callaghan, NSW, 2308, Australia
| | - Ajayan Vinu
- Global Innovative Centre for Advanced Nanomaterials (GICAN), School of Engineering, College of Engineering, Science and Environment, The University of Newcastle, Callaghan, NSW, 2308, Australia
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14
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Li B, Yu X, Lu X, Sun X, Kai Y, Cheng L, Zhou H, Tian Y, Li D. Advancing Two-Photon Photodynamic Therapy Over NIR-II Excitable Conjugated Microporous Polymer with NIR-I Emission. Adv Healthc Mater 2025; 14:e2402274. [PMID: 39460477 DOI: 10.1002/adhm.202402274] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 06/21/2024] [Revised: 10/10/2024] [Indexed: 10/28/2024]
Abstract
The availability of second near-infrared (NIR-II) excitable two-photon photosensitizers with NIR-I emission for efficient photodynamic therapy (PDT) is limited by challenges in molecular design. In this study, a NIR-II light-excitable two-photon conjugated microporous polymer (Tph-Dbd) with emission in the NIR-I region is developed. The large conjugated system and delocalized electronic structures endow Tph-Dbd with a large two-photon absorption cross-section under NIR-II light excitation. Moreover, the efficient electron acceptor and donor units within the π-conjugated backbones result in NIR-I emission for high signal-to-background ratio imaging, as well as separated highest occupied molecular orbital and lowest unoccupied molecular orbital distributions for excellent singlet oxygen generation ability. The excellent NIR-II excitable two-photon absorption activity, NIR-I emission, good biocompatibility, and high photostability allow Tph-Dbd to be used for efficient in vitro fluorescence imaging guided PDT. Moreover, the impressive photothermal effect of Tph-Dbd can overcome the limitations of PDT in the treatment of hypoxic tumors. This study highlights a strategy for designing NIR-II excitable two-photon photosensitizers for advanced PDT.
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Affiliation(s)
- Bo Li
- Institutes of Physical Science and Information Technology, Faculty of Materials Science and Engineering, School of Chemistry and Chemical Engineering, School of Life Sciences, Key Laboratory of Structure and Functional Regulation of Hybrid Materials, Ministry of Education, Anhui University, Hefei, 230601, P. R. China
| | - Xinlei Yu
- Institutes of Physical Science and Information Technology, Faculty of Materials Science and Engineering, School of Chemistry and Chemical Engineering, School of Life Sciences, Key Laboratory of Structure and Functional Regulation of Hybrid Materials, Ministry of Education, Anhui University, Hefei, 230601, P. R. China
| | - Xin Lu
- Institutes of Physical Science and Information Technology, Faculty of Materials Science and Engineering, School of Chemistry and Chemical Engineering, School of Life Sciences, Key Laboratory of Structure and Functional Regulation of Hybrid Materials, Ministry of Education, Anhui University, Hefei, 230601, P. R. China
| | - Xianshun Sun
- Institutes of Physical Science and Information Technology, Faculty of Materials Science and Engineering, School of Chemistry and Chemical Engineering, School of Life Sciences, Key Laboratory of Structure and Functional Regulation of Hybrid Materials, Ministry of Education, Anhui University, Hefei, 230601, P. R. China
| | - Yuanzhong Kai
- Institutes of Physical Science and Information Technology, Faculty of Materials Science and Engineering, School of Chemistry and Chemical Engineering, School of Life Sciences, Key Laboratory of Structure and Functional Regulation of Hybrid Materials, Ministry of Education, Anhui University, Hefei, 230601, P. R. China
| | - Longjiu Cheng
- Institutes of Physical Science and Information Technology, Faculty of Materials Science and Engineering, School of Chemistry and Chemical Engineering, School of Life Sciences, Key Laboratory of Structure and Functional Regulation of Hybrid Materials, Ministry of Education, Anhui University, Hefei, 230601, P. R. China
| | - Hongping Zhou
- Institutes of Physical Science and Information Technology, Faculty of Materials Science and Engineering, School of Chemistry and Chemical Engineering, School of Life Sciences, Key Laboratory of Structure and Functional Regulation of Hybrid Materials, Ministry of Education, Anhui University, Hefei, 230601, P. R. China
| | - Yupeng Tian
- Institutes of Physical Science and Information Technology, Faculty of Materials Science and Engineering, School of Chemistry and Chemical Engineering, School of Life Sciences, Key Laboratory of Structure and Functional Regulation of Hybrid Materials, Ministry of Education, Anhui University, Hefei, 230601, P. R. China
| | - Dandan Li
- Institutes of Physical Science and Information Technology, Faculty of Materials Science and Engineering, School of Chemistry and Chemical Engineering, School of Life Sciences, Key Laboratory of Structure and Functional Regulation of Hybrid Materials, Ministry of Education, Anhui University, Hefei, 230601, P. R. China
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15
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Lou Z, Zhao Y, Gong Z, Zhu Z, Wu M, Wang T, Wang J, Qi H, Zuo H, Xu Z, Shen J, Wang Z, Li L, Xu S, Kong W, Li W, Zheng X, Wang H, Lin X. Phase Engineering of Giant Second Harmonic Generation in Bi 2O 2Se. ADVANCED MATERIALS (DEERFIELD BEACH, FLA.) 2025; 37:e2409887. [PMID: 39632668 DOI: 10.1002/adma.202409887] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 07/09/2024] [Revised: 11/14/2024] [Indexed: 12/07/2024]
Abstract
2D materials with remarkable second-harmonic generation (SHG) hold promise for future on-chip nonlinear optics. Relevant materials with both giant SHG response and environmental stability are long-sought targets. Here, the enormous SHG from the phase engineering of a high-performance semiconductor, Bi2O2Se (BOS), under uniaxial strain, is demonstrated. SHG signals captured in strained 20 nm-BOS films exceed those of NbOI2 and NbOCl2 of similar thickness by a factor of 10, and are four orders of magnitude higher than monolayer-MoS2, resulting in a significant second-order nonlinear susceptibility on the order of 1 nm V-1. Intriguingly, the strain enables continuous adjustment of the ferroelectric phase transition across room temperature. An exceptionally large tunability of SHG, approximately six orders of magnitude, is achieved through strain modulation. This colossal SHG, originating from the geometric phase of Bloch wave functions and coupled with sensitive strain tunability in this air-stable 2D semiconductor, opens new possibilities for designing chip-scale, switchable nonlinear optical devices.
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Affiliation(s)
- Zhefeng Lou
- Key Laboratory for Quantum Materials of Zhejiang Province, Department of Physics, School of Science and Research Center for Industries of the Future, Westlake University, Hangzhou, 310030, P. R. China
- Center for Quantum Matter, School of Physics, Zhejiang University, Hangzhou, 310058, P. R. China
- Institute of Natural Sciences, Westlake Institute for Advanced Study, Hangzhou, 310024, P. R. China
| | - Yingjie Zhao
- Key Laboratory of 3D Micro/nano Fabrication and Characterization of Zhejiang Province, School of Engineering, Westlake University, Hangzhou, 310024, P. R. China
| | - Zhihao Gong
- Academy of Interdisciplinary Studies on Intelligent Molecules Tianjin Key Laboratory of Structure and Performance for Functional Molecules College of Chemistry, Tianjin Normal University, Tianjin, 300387, P. R. China
| | - Ziye Zhu
- Key Laboratory of 3D Micro/nano Fabrication and Characterization of Zhejiang Province, School of Engineering, Westlake University, Hangzhou, 310024, P. R. China
| | - Mengqi Wu
- Key Laboratory of 3D Micro/nano Fabrication and Characterization of Zhejiang Province, School of Engineering, Westlake University, Hangzhou, 310024, P. R. China
| | - Tao Wang
- Key Laboratory for Quantum Materials of Zhejiang Province, Department of Physics, School of Science and Research Center for Industries of the Future, Westlake University, Hangzhou, 310030, P. R. China
| | - Jialu Wang
- Key Laboratory for Quantum Materials of Zhejiang Province, Department of Physics, School of Science and Research Center for Industries of the Future, Westlake University, Hangzhou, 310030, P. R. China
- Hangzhou Key Laboratory of Quantum Matters School of Physics, Hangzhou Normal University, Hangzhou, 311121, P. R. China
| | - Haoyu Qi
- Key Laboratory for Quantum Materials of Zhejiang Province, Department of Physics, School of Science and Research Center for Industries of the Future, Westlake University, Hangzhou, 310030, P. R. China
- Material Science Center, Yangtze Delta Region Academy of Beijing Institute of Technology, Jiaxing, 314011, P. R. China
| | - Huakun Zuo
- Wuhan National High Magnetic Field Center, Huazhong University of Science and Technology, Wuhan, 430074, P. R. China
| | - Zhuokai Xu
- Key Laboratory for Quantum Materials of Zhejiang Province, Department of Physics, School of Science and Research Center for Industries of the Future, Westlake University, Hangzhou, 310030, P. R. China
- Center for Quantum Matter, School of Physics, Zhejiang University, Hangzhou, 310058, P. R. China
- Institute of Natural Sciences, Westlake Institute for Advanced Study, Hangzhou, 310024, P. R. China
| | - Jichuang Shen
- Key Laboratory of 3D Micro/nano Fabrication and Characterization of Zhejiang Province, School of Engineering, Westlake University, Hangzhou, 310024, P. R. China
| | - Zhiwei Wang
- Material Science Center, Yangtze Delta Region Academy of Beijing Institute of Technology, Jiaxing, 314011, P. R. China
- Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE) School of Physics, Beijing Institute of Technology, Beijing, 100081, P. R. China
- Beijing Key Lab of Nanophotonics and Ultrafine Optoelectronic Systems, Beijing Institute of Technology, Beijing, 100081, P. R. China
| | - Lan Li
- Key Laboratory of 3D Micro/nano Fabrication and Characterization of Zhejiang Province, School of Engineering, Westlake University, Hangzhou, 310024, P. R. China
| | - Shuigang Xu
- Key Laboratory for Quantum Materials of Zhejiang Province, Department of Physics, School of Science and Research Center for Industries of the Future, Westlake University, Hangzhou, 310030, P. R. China
- Institute of Natural Sciences, Westlake Institute for Advanced Study, Hangzhou, 310024, P. R. China
| | - Wei Kong
- Key Laboratory of 3D Micro/nano Fabrication and Characterization of Zhejiang Province, School of Engineering, Westlake University, Hangzhou, 310024, P. R. China
| | - Wenbin Li
- Key Laboratory of 3D Micro/nano Fabrication and Characterization of Zhejiang Province, School of Engineering, Westlake University, Hangzhou, 310024, P. R. China
| | - Xiaorui Zheng
- Key Laboratory of 3D Micro/nano Fabrication and Characterization of Zhejiang Province, School of Engineering, Westlake University, Hangzhou, 310024, P. R. China
| | - Hua Wang
- Center for Quantum Matter, School of Physics, Zhejiang University, Hangzhou, 310058, P. R. China
| | - Xiao Lin
- Key Laboratory for Quantum Materials of Zhejiang Province, Department of Physics, School of Science and Research Center for Industries of the Future, Westlake University, Hangzhou, 310030, P. R. China
- Institute of Natural Sciences, Westlake Institute for Advanced Study, Hangzhou, 310024, P. R. China
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16
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Gu S, Chen B, Xu X, Han F, Chen S. 3D Nanofabrication via Directed Material Assembly: Mechanism, Method, and Future. ADVANCED MATERIALS (DEERFIELD BEACH, FLA.) 2025; 37:e2312915. [PMID: 39623887 PMCID: PMC11733727 DOI: 10.1002/adma.202312915] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/29/2023] [Revised: 06/27/2024] [Indexed: 01/16/2025]
Abstract
Fabrication of complex three-dimensional (3D) structures at nanoscale is the core of nanotechnology, as it enables the creation of various micro-/nano-devices such as micro-robots, metamaterials, sensors, photonic devices, etc. Among most 3D nanofabrication strategies, the guided material assembly, an efficient bottom-up approach capable of directly constructing designed structures from precise integration of material building blocks, possesses compelling advantages in diverse material compatibility, sufficient driving forces, facile processing steps, and nanoscale resolution. In this review, we focus on assembly-based fabrication methods capable of creating complex 3D nanostructures (instead of periodic or 2.5D-only structures). Recent advances are classified based on the different assembly mechanisms, i.e., assembly driven by chemical reactions, physical interactions, and the synergy of multiple microscopic interactions. The design principles of representative fabrication strategies with an emphasis on their respective advantages, e.g., structural design flexibility, material compatibility, resolution, or applications are analyzed. In the summary and outlook, existing challenges, as well as possible paths to solutions for future development are reviewed. We believe that with recent advances in assembly-based nanofabrication strategies, 3D nanofabrication has achieved tremendous progress in resolution, material generality, and manufacturing cost, for it to make a greater impact in the near future.
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Affiliation(s)
- Songyun Gu
- Department of Mechanical and Automation EngineeringThe Chinese University of Hong KongShatinNew TerritoriesHong Kong SAR
| | - Bingxu Chen
- Department of Mechanical and Automation EngineeringThe Chinese University of Hong KongShatinNew TerritoriesHong Kong SAR
| | - Xiayi Xu
- Department of Mechanical and Automation EngineeringThe Chinese University of Hong KongShatinNew TerritoriesHong Kong SAR
- School of Biomedical Sciences and EngineeringGuangzhou International CampusSouth China University of TechnologyGuangzhou511442P. R. China
| | - Fei Han
- Department of Mechanical and Automation EngineeringThe Chinese University of Hong KongShatinNew TerritoriesHong Kong SAR
- School of Chemistry and Chemical EngineeringHarbin Institute of TechnologyHarbin150001P. R. China
| | - Shih‐Chi Chen
- Department of Mechanical and Automation EngineeringThe Chinese University of Hong KongShatinNew TerritoriesHong Kong SAR
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17
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Guo Q, Wu YK, Zhang D, Zhang Q, Guo GC, Alù A, Ren XF, Qiu CW. Polarization entanglement enabled by orthogonally stacked van der Waals NbOCl 2 crystals. Nat Commun 2024; 15:10461. [PMID: 39622804 PMCID: PMC11612256 DOI: 10.1038/s41467-024-54876-w] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 07/26/2024] [Accepted: 11/22/2024] [Indexed: 12/06/2024] Open
Abstract
Polarization entanglement holds significant importance for photonic quantum technologies. Recently emerging subwavelength nonlinear quantum light sources, e.g., GaP and LiNbO3 thin films, benefiting from the relaxed phase-matching constraints and volume confinement, have shown intriguing properties, such as high-dimensional hyperentanglement and robust entanglement anti-degradation. Van der Waals (vdW) NbOCl2 crystal, with strong optical nonlinearities, has emerged as a potential candidate for ultrathin quantum light sources. However, polarization entanglement is inaccessible in the NbOCl2 crystal due to its unfavorable nonlinear susceptibility tensor. Here, by leveraging the twist-stacking degree of freedom inherently in vdW systems, we showcase the preparation of polarization entanglement and quantum Bell states.
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Affiliation(s)
- Qiangbing Guo
- Department of Electrical and Computer Engineering, National University of Singapore, Singapore, Singapore.
- Centre for Advanced 2D Materials and Graphene Research Centre, National University of Singapore, Singapore, Singapore.
| | - Yun-Kun Wu
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, China
- CAS Synergetic Innovation Center of Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, China
| | - Di Zhang
- Photonics Initiative, Advanced Science Research Center, City University of New York, New York, NY, USA
- The Key Laboratory of Weak-Light Nonlinear Photonics, Ministry of Education, School of Physics and TEDA Applied Physics Institute, Nankai University, Tianjin, China
| | - Qiuhong Zhang
- School of Chemistry and Materials Science, Hangzhou Institute for Advanced Study, University of Chinese Academy of Sciences, Hangzhou, China
| | - Guang-Can Guo
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, China
- CAS Synergetic Innovation Center of Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, China
- Hefei National Laboratory, University of Science and Technology of China, Hefei, China
| | - Andrea Alù
- Photonics Initiative, Advanced Science Research Center, City University of New York, New York, NY, USA
- Physics Program, Graduate Center, City University of New York, New York, NY, USA
| | - Xi-Feng Ren
- CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei, China.
- CAS Synergetic Innovation Center of Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, China.
- Hefei National Laboratory, University of Science and Technology of China, Hefei, China.
| | - Cheng-Wei Qiu
- Department of Electrical and Computer Engineering, National University of Singapore, Singapore, Singapore.
- Centre for Advanced 2D Materials and Graphene Research Centre, National University of Singapore, Singapore, Singapore.
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18
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Tong L, Bi Y, Wang Y, Peng K, Huang X, Ju W, Peng Z, Li Z, Xu L, Lin R, Yu X, Shi W, Yu H, Sun H, Xue K, He Q, Tang M, Xu J, Zhang X, Miao J, Jariwala D, Bao W, Miao X, Wang P, Ye L. Programmable nonlinear optical neuromorphic computing with bare 2D material MoS 2. Nat Commun 2024; 15:10290. [PMID: 39604389 PMCID: PMC11603154 DOI: 10.1038/s41467-024-54776-z] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 03/27/2024] [Accepted: 11/21/2024] [Indexed: 11/29/2024] Open
Abstract
Nonlinear optical responses in two-dimensional (2D) materials can build free-space optical neuromorphic computing systems. Ensuring the high performance and the tunability of the system is essential to encode diverse functions. However, common strategies, including the integration of external electrode arrays or photonic structures with 2D materials, and barely patterned 2D materials, exhibit a contradiction between performance and tunability. Because the unique band dispersions of 2D materials can provide hidden paths to boost nonlinear responses independently, here we introduced a new free-space optical computing concept within a bare molybdenum disulfide array. This system can preserve high modulation performance with fast speed, low energy consumption, and high signal-to-noise ratio. Due to the freedom from the restrictions of fixed photonic structures, the tunability is also enhanced through the synergistic encodings of the 2D cells and the excitation pulses. The computing mechanism of transition from two-photon absorption to synergistic excited states absorption intrinsically improved the modulation capability of nonlinear optical responses, revealed from the relative transmittance modulated by a pump-probe-control strategy. Optical artificial neural network (ANN) and digital processing were demonstrated, revealing the feasibility of the free-space optical computing based on bare 2D materials toward neuromorphic applications.
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Affiliation(s)
- Lei Tong
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, Hubei, China
- Wuhan National Laboratory for Optoelectronics, Huazhong University of Science and Technology, Wuhan, Hubei, China
- Department of Electronic Engineering, Materials Science and Technology Research Center, The Chinese University of Hong Kong, Hong Kong, China
| | - Yali Bi
- Britton Chance Center for Biomedical Photonics, Wuhan National Laboratory for Optoelectronics, Huazhong University of Science and Technology, Wuhan, Hubei, China
- Anhui Province Key Laboratory of Measuring Theory and Precision Instrument, School of Instrument Science and Opto-Electronics Engineering, Hefei University of Technology, Hefei, China
| | - Yilun Wang
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, Hubei, China
| | - Kai Peng
- Department of Materials Science and Engineering, Rensselaer Polytechnic Institute, Troy, NY, USA
| | - Xinyu Huang
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, Hubei, China
| | - Wei Ju
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, Hubei, China
- Britton Chance Center for Biomedical Photonics, Wuhan National Laboratory for Optoelectronics, Huazhong University of Science and Technology, Wuhan, Hubei, China
| | - Zhuiri Peng
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, Hubei, China
| | - Zheng Li
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, Hubei, China
| | - Langlang Xu
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, Hubei, China
| | - Runfeng Lin
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, Hubei, China
| | - Xiangxiang Yu
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, Hubei, China
| | - Wenhao Shi
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, Hubei, China
| | - Hui Yu
- Department of Electronic Engineering, Materials Science and Technology Research Center, The Chinese University of Hong Kong, Hong Kong, China
| | - Huajun Sun
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, Hubei, China
- Wuhan National Laboratory for Optoelectronics, Huazhong University of Science and Technology, Wuhan, Hubei, China
| | - Kanhao Xue
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, Hubei, China
- Wuhan National Laboratory for Optoelectronics, Huazhong University of Science and Technology, Wuhan, Hubei, China
| | - Qiang He
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, Hubei, China
- Wuhan National Laboratory for Optoelectronics, Huazhong University of Science and Technology, Wuhan, Hubei, China
| | - Ming Tang
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, Hubei, China
| | - Jianbin Xu
- Department of Electronic Engineering, Materials Science and Technology Research Center, The Chinese University of Hong Kong, Hong Kong, China
| | - Xinliang Zhang
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, Hubei, China
| | - Jinshui Miao
- State Key Laboratory of Infrared Physics, Shanghai Institute of Technical Physics Chinese Academy of Sciences, Shanghai, China
| | - Deep Jariwala
- Department of Electrical and Systems Engineering, University of Pennsylvania, Philadelphia, PA, 19104, USA
| | - Wei Bao
- Department of Materials Science and Engineering, Rensselaer Polytechnic Institute, Troy, NY, USA.
| | - Xiangshui Miao
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, Hubei, China.
- Wuhan National Laboratory for Optoelectronics, Huazhong University of Science and Technology, Wuhan, Hubei, China.
| | - Ping Wang
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, Hubei, China.
- Britton Chance Center for Biomedical Photonics, Wuhan National Laboratory for Optoelectronics, Huazhong University of Science and Technology, Wuhan, Hubei, China.
| | - Lei Ye
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, Hubei, China.
- Wuhan National Laboratory for Optoelectronics, Huazhong University of Science and Technology, Wuhan, Hubei, China.
- State Key Laboratory of Infrared Physics, Shanghai Institute of Technical Physics Chinese Academy of Sciences, Shanghai, China.
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19
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Huang Y, Wang J, Bai B, Zhao M, Zhen X, Zhao L, Zhai X, Zhao L, Leng X. Dimension-Dependent Nonlinear Optical Properties of Stanene Nanosheets. ACS APPLIED MATERIALS & INTERFACES 2024; 16:59022-59029. [PMID: 39413415 DOI: 10.1021/acsami.4c10938] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 10/18/2024]
Abstract
Stanene (Sn)-based materials, with a graphene-like hexagonal structure, are now attracting considerable interest for potential applications in photoelectricity. However, the nonlinear optical properties of stanene remain largely unexplored. In this work, we prepared different sizes of stanene by liquid phase exfoliation and differential centrifugation methods, including two-dimensional (2D) Sn nanosheets (NSs) and zero-dimensional (0D) Sn nanodots (NDs). Z-scan measurements reveal that 2D Sn NSs exhibited high saturable absorption behavior, while the 0D Sn NDs led to reverse saturable absorption. Femtosecond ultrafast transient absorption spectra revealed that the reverse saturable absorption of Sn NDs is derived from a stronger excited state absorption and faster exciton relaxation dynamics. This research expands the potential applications of stanene in laser shielding and other ultrafast photonics technologies.
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Affiliation(s)
- Yifan Huang
- Institute of Special Environment Physical Sciences, Harbin Institute of Technology, Shenzhen 518055, China
| | - Jingkun Wang
- Key Laboratory of Interface Science and Engineering in Advanced Materials, Ministry of Education, Taiyuan University of Technology, Taiyuan 030024, P. R. China
| | - Bowen Bai
- Institute of Special Environment Physical Sciences, Harbin Institute of Technology, Shenzhen 518055, China
| | - Min Zhao
- Key Laboratory of Interface Science and Engineering in Advanced Materials, Ministry of Education, Taiyuan University of Technology, Taiyuan 030024, P. R. China
| | - Xiaojuan Zhen
- School of Electronic and Information Engineering, Lanzhou City University, Lanzhou 730000, P. R. China
| | - Lei Zhao
- School of Electronic and Information Engineering, Lanzhou City University, Lanzhou 730000, P. R. China
| | - Xinping Zhai
- Research Institute of Microscale Optoelectronics, School of Jia Yang, Zhejiang Shuren University, Shaoxing 312028, China
| | - Lin Zhao
- Institute of Special Environment Physical Sciences, Harbin Institute of Technology, Shenzhen 518055, China
| | - Xuesong Leng
- Institute of Special Environment Physical Sciences, Harbin Institute of Technology, Shenzhen 518055, China
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20
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Puri S, Patel S, Cabellos JL, Rosas-Hernandez LE, Reynolds K, Churchill HOH, Barraza-Lopez S, Mendoza BS, Nakamura H. Substrate Interference and Strain in the Second-Harmonic Generation from MoSe 2 Monolayers. NANO LETTERS 2024; 24. [PMID: 39356872 PMCID: PMC11487631 DOI: 10.1021/acs.nanolett.4c03880] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/13/2024] [Revised: 09/26/2024] [Accepted: 09/27/2024] [Indexed: 10/04/2024]
Abstract
Nonlinear optical materials of atomic thickness, such as non-centrosymmetric 2H transition metal dichalcogenide monolayers, have a second-order nonlinear susceptibility (χ(2)) whose intensity can be tuned by strain. However, whether χ(2) is enhanced or reduced by tensile strain is a subject of conflicting reports. Here, we grow high-quality MoSe2 monolayers under controlled biaxial strain created by two different substrates and study their linear and nonlinear optical responses with a combination of experimental and theoretical approaches. Up to a 15-fold overall enhancement in second-harmonic generation (SHG) intensity is observed from MoSe2 monolayers grown on SiO2 when compared to its value on a Si3N4 substrate. By considering an interference contribution from different dielectrics and their thicknesses, a factor of 2 enhancement of χ(2) was attributed to the biaxial strain: substrate interference and strain are independent handles to engineer the SHG strength of non-centrosymmetric 2D materials.
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Affiliation(s)
- Sudeep Puri
- Department
of Physics, University of Arkansas, Fayetteville, Arkansas 72701, United States
| | - Sneha Patel
- Department
of Physics, University of Arkansas, Fayetteville, Arkansas 72701, United States
| | - Jose Luis Cabellos
- Universidad
Politécnica de Tapachula, Tapachula, Chiapas C.P. 30830, Mexico
| | | | - Katlin Reynolds
- Department
of Physics, University of Arkansas, Fayetteville, Arkansas 72701, United States
| | - Hugh O. H. Churchill
- Department
of Physics, University of Arkansas, Fayetteville, Arkansas 72701, United States
| | - Salvador Barraza-Lopez
- Department
of Physics, University of Arkansas, Fayetteville, Arkansas 72701, United States
| | - Bernardo S. Mendoza
- Centro
de Investigaciones en Optica, A.C., León, Guanajuato C.P. 37150, Mexico
- Max
Planck Institute for the Structure and Dynamics of Matter, 22761 Hamburg, Germany
| | - Hiroyuki Nakamura
- Department
of Physics, University of Arkansas, Fayetteville, Arkansas 72701, United States
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21
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Liu X, Wu LM, Kang L, Lin Z, Chen L. Theoretical Prediction of Monolayer BeP 2O 4H 4 with Excellent Nonlinear-Optical Properties in Deep-Ultraviolet Range. SMALL (WEINHEIM AN DER BERGSTRASSE, GERMANY) 2024; 20:e2404155. [PMID: 38855996 DOI: 10.1002/smll.202404155] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 05/22/2024] [Indexed: 06/11/2024]
Abstract
Most 2D nonlinear optical (NLO) materials do not have an ultrawide bandgap, therefore, they are unsuitable for working in the deep-ultraviolet spectral range (< 200 nm). Herein, the theoretical prediction of an excellent monolayer BeP2O4H4 (ML-BPOH) is reported. DFT analyses suggest a low cleavage energy (≈45 meV per atom) from a naturally existed bulk-BPOH material, indicating feasible exfoliation. This novel 2D material exhibits excellent properties including an ultrawide bandgap (Eg) of 7.84 eV, and a strong second-order nonlinear susceptibility (d b u l k e f f $d_{bulk}^{eff}$ = 0.43 pm V-1), which is comparable to that of benchmark bulk-KBBF crystal (d16 = 0.45 pm V-1). The wide bandgap and large SHG effect of ML-BPOH are mainly derived from the (PO2H2)- tetrahedron. Notably, ML-BPOH exhibits an outstanding 50% variation in dsheet under minor stress stimuli (±3%) due to rotation of structurally rigid (PO2H2)- tetrahedron. This indicates significant potential for application in material deformation monitoring.
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Affiliation(s)
- Xin Liu
- Beijing Key Laboratory of Energy Conversion and Storage Materials, College of Chemistry, Beijing Normal University, Beijing, 100875, P. R. China
| | - Li-Ming Wu
- Beijing Key Laboratory of Energy Conversion and Storage Materials, College of Chemistry, Beijing Normal University, Beijing, 100875, P. R. China
- Center for Advanced Materials Research, Beijing Normal University, Zhuhai, 519087, P. R. China
| | - Lei Kang
- Functional Crystals Lab, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing, 100190, P. R. China
| | - Zheshuai Lin
- Functional Crystals Lab, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing, 100190, P. R. China
| | - Ling Chen
- Beijing Key Laboratory of Energy Conversion and Storage Materials, College of Chemistry, Beijing Normal University, Beijing, 100875, P. R. China
- Center for Advanced Materials Research, Beijing Normal University, Zhuhai, 519087, P. R. China
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22
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Xie J, Cheng X, Xue G, Li X, Zhong D, Yu W, Zuo Y, Liu C, Lin K, Liu C, Pang M, Jiang X, Sun Z, Kang Z, Hong H, Liu K, Liu Z. Critical-Layered MoS 2 for the Enhancement of Supercontinuum Generation in Photonic Crystal Fibre. ADVANCED MATERIALS (DEERFIELD BEACH, FLA.) 2024; 36:e2403696. [PMID: 39183501 DOI: 10.1002/adma.202403696] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/12/2024] [Revised: 06/15/2024] [Indexed: 08/27/2024]
Abstract
Supercontinuum generation (SCG) from silica-based photonic crystal fibers (PCFs) is of highly technological significance from microscopy to metrology, but has been hindered by silica's relatively low intrinsic optical nonlinearity. The prevailing approaches of filling PCF with nonlinear gases or liquids can endow fibre with enhanced optical nonlinearity and boosted SCG efficiency, yet these hybrids are easily plagued by fusion complexity, environmental incompatibility or transmission mode instability. Here this work presents a strategy of embedding solid-state 2D MoS2 atomic layers into the air-holes of PCF to efficiently enhance SCG. This work demonstrates a 4.8 times enhancement of the nonlinear coefficient and a 70% reduction of the threshold power for SCG with one octave spanning in the MoS2-PCF hybrid. Furthermore, this work finds that the SCG enhancement is highly layer-dependent, which only manifests for a real 2D regime within the thickness of five atomic layers. Theoretical calculations reveal that the critical thickness arises from the trade-off among the layer-dependent enhancement of the nonlinear coefficient, leakage of fundamental mode and redshift of zero-dispersion wavelength. This work provides significant advances toward efficient SCG, and highlights the importance of matching an appropriate atomic layer number in the design of functional 2D material optical fibers.
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Affiliation(s)
- Jin Xie
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, Beijing, 100871, China
- Academy for Advanced Interdisciplinary Studies, Peking University, Beijing, 100871, China
- Beijing Graphene Institute (BGI), Beijing, 100095, China
| | - Xu Cheng
- Group for Fibre Optics, École Polytechnique Fédérale de Lausanne (EPFL), Lausanne, 1015, Switzerland
- Haute Ecole ARC Ingénierie, University of Applied Sciences of Western Switzerland, Saint-Imier, 2610, Switzerland
| | - Guodong Xue
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, Beijing, 100871, China
- Academy for Advanced Interdisciplinary Studies, Peking University, Beijing, 100871, China
| | - Xiao Li
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, Beijing, 100871, China
- Academy for Advanced Interdisciplinary Studies, Peking University, Beijing, 100871, China
| | - Ding Zhong
- Department of Physics, Renmin University of China, Beijing, 100872, China
| | - Wentao Yu
- Institute of Interdisciplinary Physical Sciences, School of Physics, Nanjing University of Science and Technology, Nanjing, 210094, China
| | - Yonggang Zuo
- Faculty of Metallurgical and Energy Engineering, Kunming University of Science and Technology, Kunming, 650093, China
| | - Chang Liu
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, Beijing, 100871, China
| | - Kaifeng Lin
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, Beijing, 100871, China
- Academy for Advanced Interdisciplinary Studies, Peking University, Beijing, 100871, China
| | - Can Liu
- Department of Physics, Renmin University of China, Beijing, 100872, China
| | - Meng Pang
- Innovation and Integration Center of New Laser Technology, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai, 201800, China
- Russell Centre for Advanced Lightwave Science, Shanghai Institute of Optics and Fine Mechanics and Hangzhou Institute of Optics and Fine Mechanics, Hangzhou, 311421, China
| | - Xin Jiang
- Innovation and Integration Center of New Laser Technology, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai, 201800, China
- Russell Centre for Advanced Lightwave Science, Shanghai Institute of Optics and Fine Mechanics and Hangzhou Institute of Optics and Fine Mechanics, Hangzhou, 311421, China
| | - Zhipei Sun
- QTF Center of Excellence, Department of Electronics and Nanoengineering, Aalto University, Espoo, 02150, Finland
| | - Zhe Kang
- Centre for Optical and Electromagnetic Research, College of Optical Science and Engineering, National Engineering Research Center for Optical Instruments, Ningbo Innovation Center, Zhejiang University, Hangzhou, 310058, China
| | - Hao Hong
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, Beijing, 100871, China
- Interdisciplinary Institute of Light-Element Quantum Materials and Research Centre for Light-Element Advanced Materials, Peking University, Beijing, 100871, China
| | - Kaihui Liu
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, Beijing, 100871, China
- Songshan Lake Materials Lab, Institute of Physics, Chinese Academy of Sciences, Dongguan, 523808, China
| | - Zhongfan Liu
- Beijing Graphene Institute (BGI), Beijing, 100095, China
- Center for Nanochemistry, College of Chemistry and Molecular Engineering, Peking University, Beijing, 100871, China
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23
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Xue G, Qin B, Ma C, Yin P, Liu C, Liu K. Large-Area Epitaxial Growth of Transition Metal Dichalcogenides. Chem Rev 2024; 124:9785-9865. [PMID: 39132950 DOI: 10.1021/acs.chemrev.3c00851] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 08/13/2024]
Abstract
Over the past decade, research on atomically thin two-dimensional (2D) transition metal dichalcogenides (TMDs) has expanded rapidly due to their unique properties such as high carrier mobility, significant excitonic effects, and strong spin-orbit couplings. Considerable attention from both scientific and industrial communities has fully fueled the exploration of TMDs toward practical applications. Proposed scenarios, such as ultrascaled transistors, on-chip photonics, flexible optoelectronics, and efficient electrocatalysis, critically depend on the scalable production of large-area TMD films. Correspondingly, substantial efforts have been devoted to refining the synthesizing methodology of 2D TMDs, which brought the field to a stage that necessitates a comprehensive summary. In this Review, we give a systematic overview of the basic designs and significant advancements in large-area epitaxial growth of TMDs. We first sketch out their fundamental structures and diverse properties. Subsequent discussion encompasses the state-of-the-art wafer-scale production designs, single-crystal epitaxial strategies, and techniques for structure modification and postprocessing. Additionally, we highlight the future directions for application-driven material fabrication and persistent challenges, aiming to inspire ongoing exploration along a revolution in the modern semiconductor industry.
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Affiliation(s)
- Guodong Xue
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, Beijing 100871, China
- Academy for Advanced Interdisciplinary Studies, Peking University, Beijing 100871, China
| | - Biao Qin
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, Beijing 100871, China
| | - Chaojie Ma
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, Beijing 100871, China
| | - Peng Yin
- Key Laboratory of Quantum State Construction and Manipulation (Ministry of Education), Department of Physics, Renmin University of China, Beijing 100872, China
| | - Can Liu
- Key Laboratory of Quantum State Construction and Manipulation (Ministry of Education), Department of Physics, Renmin University of China, Beijing 100872, China
| | - Kaihui Liu
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, Beijing 100871, China
- International Centre for Quantum Materials, Collaborative Innovation Centre of Quantum Matter, Peking University, Beijing 100871, China
- Songshan Lake Materials Laboratory, Dongguan 523808, China
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24
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Du L, Huang Z, Zhang J, Ye F, Dai Q, Deng H, Zhang G, Sun Z. Nonlinear physics of moiré superlattices. NATURE MATERIALS 2024; 23:1179-1192. [PMID: 39215154 DOI: 10.1038/s41563-024-01951-8] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/16/2023] [Accepted: 06/13/2024] [Indexed: 09/04/2024]
Abstract
Nonlinear physics is one of the most important research fields in modern physics and materials science. It offers an unprecedented paradigm for exploring many fascinating physical phenomena and realizing diverse cutting-edge applications inconceivable in the framework of linear processes. Here we review the recent theoretical and experimental progress concerning the nonlinear physics of synthetic quantum moiré superlattices. We focus on the emerging nonlinear electronic, optical and optoelectronic properties of moiré superlattices, including but not limited to the nonlinear anomalous Hall effect, dynamically twistable harmonic generation, nonlinear optical chirality, ultralow-power-threshold optical solitons and spontaneous photogalvanic effect. We also present our perspectives on the future opportunities and challenges in this rapidly progressing field, and highlight the implications for advances in both fundamental physics and technological innovations.
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Affiliation(s)
- Luojun Du
- Beijing National Laboratory for Condensed Matter Physics, Key Laboratory for Nanoscale Physics and Devices, Institute of Physics, Chinese Academy of Sciences, Beijing, China.
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, China.
| | - Zhiheng Huang
- Beijing National Laboratory for Condensed Matter Physics, Key Laboratory for Nanoscale Physics and Devices, Institute of Physics, Chinese Academy of Sciences, Beijing, China
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, China
| | - Jin Zhang
- QTF Centre of Excellence, Department of Electronics and Nanoengineering, Aalto University, Espoo, Finland
| | - Fangwei Ye
- State Key Laboratory of Advanced Optical Communication Systems and Networks, School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai, China
| | - Qing Dai
- CAS Key Laboratory of Nanophotonic Materials and Devices, CAS Key Laboratory of Standardization and Measurement for Nanotechnology, CAS Center for Excellence in Nanoscience, National Center for Nanoscience and Technology, Beijing, China
- School of Materials Science and Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Hui Deng
- Physics Department, University of Michigan, Ann Arbor, MI, USA
| | - Guangyu Zhang
- Beijing National Laboratory for Condensed Matter Physics, Key Laboratory for Nanoscale Physics and Devices, Institute of Physics, Chinese Academy of Sciences, Beijing, China.
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, China.
- Songshan-Lake Materials Laboratory, Dongguan, China.
| | - Zhipei Sun
- QTF Centre of Excellence, Department of Electronics and Nanoengineering, Aalto University, Espoo, Finland.
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25
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Ma C, Ma C, Liu C, Guo Q, Huang C, Yao G, Li M, Qi J, Qin B, Sui X, Li J, Wu M, Gao P, Wang W, Bai X, Sun Z, Wang E, Hong H, Liu K. Strong chiroptical nonlinearity in coherently stacked boron nitride nanotubes. NATURE NANOTECHNOLOGY 2024; 19:1299-1305. [PMID: 38844662 DOI: 10.1038/s41565-024-01685-3] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/22/2023] [Accepted: 04/24/2024] [Indexed: 09/18/2024]
Abstract
Nanomaterials with a large chiroptical response and high structural stability are desirable for advanced miniaturized optical and optoelectronic applications. One-dimensional (1D) nanotubes are robust crystals with inherent and continuously tunable chiral geometries. However, their chiroptical response is typically weak and hard to control, due to the diverse structures of the coaxial tubes. Here we demonstrate that as-grown multiwalled boron nitride nanotubes (BNNTs), featuring coherent-stacking structures including near monochirality, homo-handedness and unipolarity among the component tubes, exhibit a scalable nonlinear chiroptical response. This intrinsic architecture produces a strong nonlinear optical response in individual multiwalled BNNTs, enabling second-harmonic generation (SHG) with a conversion efficiency up to 0.01% and output power at the microwatt level-both excellent figures of merit in the 1D nanomaterials family. We further show that the rich chirality of the nanotubes introduces a controllable nonlinear geometric phase, producing a chirality-dependent SHG circular dichroism with values of -0.7 to +0.7. We envision that our 1D chiral platform will enable novel functions in compact nonlinear light sources and modulators.
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Affiliation(s)
- Chaojie Ma
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China
| | - Chenjun Ma
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China
| | - Chang Liu
- International Centre for Quantum Materials, Collaborative Innovation Centre of Quantum Matter, Peking University, Beijing, China
| | - Quanlin Guo
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China
| | - Chen Huang
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China
| | - Guangjie Yao
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China
| | - Meiyun Li
- Institute of Physics, Chinese Academy of Sciences, Beijing, China
| | - Jiajie Qi
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China
| | - Biao Qin
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China
| | - Xin Sui
- International Centre for Quantum Materials, Collaborative Innovation Centre of Quantum Matter, Peking University, Beijing, China
| | - Jiacheng Li
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China
| | - Muhong Wu
- International Centre for Quantum Materials, Collaborative Innovation Centre of Quantum Matter, Peking University, Beijing, China
| | - Peng Gao
- International Centre for Quantum Materials, Collaborative Innovation Centre of Quantum Matter, Peking University, Beijing, China
| | - Wenlong Wang
- Institute of Physics, Chinese Academy of Sciences, Beijing, China
- Songshan Lake Materials Laboratory, Institute of Physics, Chinese Academy of Sciences, Dongguan, China
| | - Xuedong Bai
- Institute of Physics, Chinese Academy of Sciences, Beijing, China
- Songshan Lake Materials Laboratory, Institute of Physics, Chinese Academy of Sciences, Dongguan, China
| | - Zhipei Sun
- QTF Centre of Excellence, Department of Electronics and Nanoengineering, Aalto University, Espoo, Finland
| | - Enge Wang
- International Centre for Quantum Materials, Collaborative Innovation Centre of Quantum Matter, Peking University, Beijing, China
- Songshan Lake Materials Laboratory, Institute of Physics, Chinese Academy of Sciences, Dongguan, China
- School of Physics, Liaoning University, Shenyang, China
| | - Hao Hong
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China.
- Interdisciplinary Institute of Light-Element Quantum Materials and Research Centre for Light-Element Advanced Materials, Peking University, Beijing, China.
| | - Kaihui Liu
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China.
- International Centre for Quantum Materials, Collaborative Innovation Centre of Quantum Matter, Peking University, Beijing, China.
- Songshan Lake Materials Laboratory, Institute of Physics, Chinese Academy of Sciences, Dongguan, China.
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26
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Liu Z, Chen B, Wang X, Qiu G, Cao Q, Wei D, Liu J. Enhanced vertical second harmonic generation from layered GaSe coupled to photonic crystal circular Bragg resonators. NANOPHOTONICS (BERLIN, GERMANY) 2024; 13:4029-4035. [PMID: 39634950 PMCID: PMC11501048 DOI: 10.1515/nanoph-2024-0282] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 05/25/2024] [Accepted: 07/28/2024] [Indexed: 12/07/2024]
Abstract
Two-dimensional (2D) layered materials without centrosymmetry, such as GaSe, have emerged as promising novel optical materials due to large second-order nonlinear susceptibilities. However, their nonlinear responses are severely limited by the short interaction between the 2D materials and light, which should be improved by coupling them with photonic structures with strong field confinement. Here, we theoretically design photonic crystal circular Bragg gratings (CBG) based on hole gratings with a quality factor as high as Q = 8 × 103, a mode volume as small as V = 1.18 (λ/n)3, and vertical emission of light field in silicon nitride thin film platform. Experimentally, we achieved a Q value up to nearly 4 × 103, resulting in a 1,200-fold enhancement of second harmonic generation from GaSe flakes with a thickness of 50 nm coupling to the CBG structures under continuous-wave excitation. Our work endows silicon-based photonic platforms with significant second-order nonlinear effect, which is potentially applied in on-chip quantum light sources and nonlinear frequency conversion.
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Affiliation(s)
- Zhuojun Liu
- State Key Laboratory for Mesoscopic Physics and Frontiers Science Center for Nano-Optoelectronics, School of Physics, Peking University, Beijing100871, China
| | - Bo Chen
- State Key Laboratory of Optoelectronic Materials and Technologies, School of Physics, School of Electronics and Information Technology, Sun Yat-Sen University, Guangzhou510275, China
| | - Xuying Wang
- State Key Laboratory of Optoelectronic Materials and Technologies, School of Physics, School of Electronics and Information Technology, Sun Yat-Sen University, Guangzhou510275, China
| | - Guixin Qiu
- State Key Laboratory of Optoelectronic Materials and Technologies, School of Physics, School of Electronics and Information Technology, Sun Yat-Sen University, Guangzhou510275, China
| | - Qitao Cao
- State Key Laboratory for Mesoscopic Physics and Frontiers Science Center for Nano-Optoelectronics, School of Physics, Peking University, Beijing100871, China
| | - Dunzhao Wei
- State Key Laboratory of Optoelectronic Materials and Technologies, School of Physics, School of Electronics and Information Technology, Sun Yat-Sen University, Guangzhou510275, China
| | - Jin Liu
- State Key Laboratory of Optoelectronic Materials and Technologies, School of Physics, School of Electronics and Information Technology, Sun Yat-Sen University, Guangzhou510275, China
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27
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Qian C, Villafañe V, Soubelet P, Ji P, Stier AV, Finley JJ. Probing Dark Excitons in Monolayer MoS_{2} by Nonlinear Two-Photon Spectroscopy. PHYSICAL REVIEW LETTERS 2024; 133:086902. [PMID: 39241713 DOI: 10.1103/physrevlett.133.086902] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/30/2023] [Revised: 03/28/2024] [Accepted: 07/25/2024] [Indexed: 09/09/2024]
Abstract
We report a new dark exciton in monolayer MoS_{2} using second harmonic generation spectroscopy. Hereby, the spectrally dependent second harmonic generation intensity splits into two branches, and an anticrossing is observed at ∼25 meV blue detuned from the bright neutral exciton. These observations are indicative of coherent quantum interference arising from strong two-photon light-matter interaction with an excitonic state that is dark for single photon interaction. The existence of the dark state is supported by engineering its relaxation to bright localized excitons, mediated by vibrational modes of a proximal nanobeam cavity. We show that two-photon light-matter interaction involving dark states has the potential to control relaxation pathways induced by nanostructuring the local environment. Moreover, our results indicate that dark excitons have significant potential for nonlinear quantum devices based on their nontrivial excitonic photophysics.
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Affiliation(s)
- Chenjiang Qian
- Walter Schottky Institut and TUM School of Natural Sciences, Technische Universität München, Am Coulombwall 4, 85748 Garching, Germany
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China
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28
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Jelić JZ, Bukumira M, Denčevski A, Senkić A, Žužić L, Radatović B, Vujičić N, Pajić T, Rabasović MD, Krmpot AJ. Application of the Knife-Edge Technique on Transition Metal Dichalcogenide Monolayers for Resolution Assessment of Nonlinear Microscopy Modalities. MICROSCOPY AND MICROANALYSIS : THE OFFICIAL JOURNAL OF MICROSCOPY SOCIETY OF AMERICA, MICROBEAM ANALYSIS SOCIETY, MICROSCOPICAL SOCIETY OF CANADA 2024; 30:671-680. [PMID: 38993166 DOI: 10.1093/mam/ozae061] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 02/05/2024] [Revised: 06/19/2024] [Accepted: 06/23/2024] [Indexed: 07/13/2024]
Abstract
We report application of the knife-edge technique at the sharp edges of WS2 and MoS2 monolayer flakes for lateral and axial resolution assessment in all three modalities of nonlinear laser scanning microscopy: two-photon excited fluorescence (TPEF), second- and third-harmonic generation (SHG, THG) imaging. This technique provides a high signal-to-noise ratio, no photobleaching effect and shows good agreement with standard resolution measurement techniques. Furthermore, we assessed both the lateral resolution in TPEF imaging modality and the axial resolution in SHG and THG imaging modality directly via the full-width at half maximum parameter of the corresponding Gaussian distribution. We comprehensively analyzed the factors influencing the resolution, such as the numerical aperture, the excitation wavelength and the refractive index of the embedding medium for the different imaging modalities. Glycerin was identified as the optimal embedding medium for achieving resolutions closest to the theoretical limit. The proposed use of WS2 and MoS2 monolayer flakes emerged as promising tools for characterization of nonlinear imaging systems.
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Affiliation(s)
- Jovana Z Jelić
- Institute of Physics Belgrade, University of Belgrade, National Institute of the Republic of Serbia, Pregrevica 118, Belgrade 11080, Serbia
| | - Marta Bukumira
- Institute of Physics Belgrade, University of Belgrade, National Institute of the Republic of Serbia, Pregrevica 118, Belgrade 11080, Serbia
| | - Aleksa Denčevski
- Institute of Physics Belgrade, University of Belgrade, National Institute of the Republic of Serbia, Pregrevica 118, Belgrade 11080, Serbia
| | - Ana Senkić
- Centre for Advanced Laser Techniques, Institute of Physics Zagreb, Bijenička cesta 46, Zagreb 10000, Croatia
| | - Livio Žužić
- Department of Physics, University of Zagreb, Bijenička cesta 32, Zagreb 10000, Croatia
| | - Borna Radatović
- Materials Science Factory, Instituto de Ciencia de Materiales de Madrid (ICMM-CSIC), Sor Juana Ines de la Cruz 3, Madrid 28049, Spain
| | - Nataša Vujičić
- Centre for Advanced Laser Techniques, Institute of Physics Zagreb, Bijenička cesta 46, Zagreb 10000, Croatia
| | - Tanja Pajić
- Department for General Physiology and Biophysics, Faculty of Biology, University of Belgrade, Studentski trg 16, Belgrade, 11158, Serbia
| | - Mihailo D Rabasović
- Institute of Physics Belgrade, University of Belgrade, National Institute of the Republic of Serbia, Pregrevica 118, Belgrade 11080, Serbia
| | - Aleksandar J Krmpot
- Institute of Physics Belgrade, University of Belgrade, National Institute of the Republic of Serbia, Pregrevica 118, Belgrade 11080, Serbia
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29
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Yue L, Liu C, Han S, Hong H, Wang Y, Liu Q, Qi J, Li Y, Wu D, Liu K, Wang E, Dong T, Wang N. Giant nonlinear optical wave mixing in a van der Waals correlated insulator. SCIENCE ADVANCES 2024; 10:eadn6216. [PMID: 39093978 PMCID: PMC11296339 DOI: 10.1126/sciadv.adn6216] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 12/21/2023] [Accepted: 06/28/2024] [Indexed: 08/04/2024]
Abstract
Optical nonlinearities are one of the most fascinating properties of two-dimensional (2D) materials. While tremendous efforts have been made to find and optimize the second-order optical nonlinearity in enormous 2D materials, opportunities to explore higher-order ones are elusive because of the much lower efficiency. Here, we report the giant high odd-order optical nonlinearities in centrosymmetric correlated van der Waals insulator manganese phosphorus triselenide. When illuminated by two near-infrared femtosecond lasers, the sample generates a series of profound four- and six-wave mixing outputs. The near-infrared third-order nonlinear susceptibility reaches near the highest record values of 2D materials. Comparative measurements to other prototypical nonlinear optical materials [lithium niobate, gallium(II) selenide, and tungsten disulfide] reveal its extraordinary wave mixing efficiency. The wave mixing processes are further used for nonlinear optical waveguide with multicolor emission. Our work highlights the promising prospect for future research of the nonlinear light-matter interactions in the correlated 2D system and for potential nonlinear photonic applications.
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Affiliation(s)
- Li Yue
- International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China
- Beijing Academy of Quantum Information Sciences, Beijing 100193, China
| | - Chang Liu
- International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China
| | - Shanshan Han
- Beijing Academy of Quantum Information Sciences, Beijing 100193, China
- School of Materials Science and Engineering, Smart Sensing Interdisciplinary Science Center, Collaborative Innovation Center ofChemical Science and Engineering, Nankai University, Tianjin 300350, China
| | - Hao Hong
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, Beijing 100871, China
| | - Yijun Wang
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, Beijing 100871, China
| | - Qiaomei Liu
- International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China
| | - Jiajie Qi
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, Beijing 100871, China
| | - Yuan Li
- International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China
- Collaborative Innovation Center of Quantum Matter, Beijing, China
| | - Dong Wu
- Beijing Academy of Quantum Information Sciences, Beijing 100193, China
| | - Kaihui Liu
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, Beijing 100871, China
| | - Enge Wang
- International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China
- Collaborative Innovation Center of Quantum Matter, Beijing, China
| | - Tao Dong
- International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China
| | - Nanlin Wang
- International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China
- Beijing Academy of Quantum Information Sciences, Beijing 100193, China
- Collaborative Innovation Center of Quantum Matter, Beijing, China
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30
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Ren P, Huang Z, Luo S, Liu J, Dong X, Zhang H, Li J, Yang Z. Quasi-BICs enhanced second harmonic generation from WSe 2 monolayer. NANOPHOTONICS (BERLIN, GERMANY) 2024; 13:3449-3456. [PMID: 39634849 PMCID: PMC11501586 DOI: 10.1515/nanoph-2024-0108] [Citation(s) in RCA: 1] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 03/05/2024] [Accepted: 05/20/2024] [Indexed: 12/07/2024]
Abstract
Quasi-bound states in the continuum (quasi-BICs) offer unique advantages in enhancing nonlinear optical processes and advancing the development of active optical devices. Here, the tunable robust quasi-BICs resonances are experimentally achieved through the engineering of multiple-hole Si-metasurface. Notably, the quasi-BICs mode exhibits flat bands with minimal dispersion at a wide range of incident angles, as demonstrated by the angle-resolved spectroscopy measurements. Furthermore, we demonstrate a giant second-harmonic generation (SHG) enhancement by coupling a WSe2 monolayer to the quasi-BICs hosted in the metasurface. Leveraging the strong local electric field and high state density of the observed quasi-BICs, the SHG from the WSe2 monolayer can be enhanced by more than two orders of magnitude. Our work paves the way for effectively enhancing nonlinear optical processes in two dimensional (2D) materials within the framework of silicon photonics and is expected to be applied in nonlinear optical devices.
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Affiliation(s)
- Peiwen Ren
- College of Physical Science and Technology, State Key Laboratory of Physical Chemistry of Solid Surfaces, Xiamen University, Xiamen361005, China
| | - Zhuo Huang
- College of Chemistry and Chemical Engineering, State Key Laboratory of Physical Chemistry of Solid Surfaces, Xiamen University, Xiamen361005, China
| | - Song Luo
- College of Physical Science and Technology, State Key Laboratory of Physical Chemistry of Solid Surfaces, Xiamen University, Xiamen361005, China
| | - Jia Liu
- College of Chemistry and Chemical Engineering, State Key Laboratory of Physical Chemistry of Solid Surfaces, Xiamen University, Xiamen361005, China
| | - Xiaoxiang Dong
- College of Physical Science and Technology, State Key Laboratory of Physical Chemistry of Solid Surfaces, Xiamen University, Xiamen361005, China
| | - Hua Zhang
- College of Chemistry and Chemical Engineering, State Key Laboratory of Physical Chemistry of Solid Surfaces, Xiamen University, Xiamen361005, China
| | - Jianfeng Li
- College of Chemistry and Chemical Engineering, State Key Laboratory of Physical Chemistry of Solid Surfaces, Xiamen University, Xiamen361005, China
| | - Zhilin Yang
- College of Physical Science and Technology, State Key Laboratory of Physical Chemistry of Solid Surfaces, Xiamen University, Xiamen361005, China
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31
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Psilodimitrakopoulos S, Ilin S, Zelenkov LE, Makarov S, Stratakis E. Tailoring of the polarization-resolved second harmonic generation in two-dimensional semiconductors. NANOPHOTONICS (BERLIN, GERMANY) 2024; 13:3181-3206. [PMID: 39634826 PMCID: PMC11501150 DOI: 10.1515/nanoph-2024-0267] [Citation(s) in RCA: 1] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 05/15/2024] [Accepted: 07/08/2024] [Indexed: 12/07/2024]
Abstract
Second harmonic generation is a non-linear optical phenomenon in which coherent radiation with frequency ω interacts with a non-centrosymmetric material and produces coherent radiation at frequency 2ω. Owing to the exciting physical phenomena that take place during the non-linear optical excitation at the nanoscale, there is currently extensive research in the non-linear optical responses of nanomaterials, particularly in low-dimensional materials. Here, we review recent advancements in the polarization-resolved second harmonic generation propertied from atomically thin two-dimensional (2D) crystals and present a unified theoretical framework to account for their nonlinear optical response. Two major classes of 2D materials are particularly investigated, namely metal chalcogenides and perovskites. The first attempts to tune and control the second harmonic generation properties of such materials via the application of specific nanophotonic schemes are additionally demonstrated and discussed. Besides presenting recent advances in the field, this work also delineates existing limitations and highlights emerging possibilities and future prospects in this field.
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Affiliation(s)
- Sotiris Psilodimitrakopoulos
- Qingdao Innovation and Development Center, Harbin Engineering University, Qingdao, China
- Foundation for Research and Technology-Hellas (FO.R.T.H), Heraklion, Crete, Greece
| | | | - Lev E. Zelenkov
- Qingdao Innovation and Development Center, Harbin Engineering University, Qingdao, China
- ITMO University, Saint Petersburg, Russia
| | - Sergey Makarov
- Qingdao Innovation and Development Center, Harbin Engineering University, Qingdao, China
- ITMO University, Saint Petersburg, Russia
| | - Emmanuel Stratakis
- Qingdao Innovation and Development Center, Harbin Engineering University, Qingdao, China
- Foundation for Research and Technology-Hellas (FO.R.T.H), Heraklion, Crete, Greece
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32
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Chu L, Li Z, Zhu H, Lv H, Chen F. Intense second-harmonic generation in two-dimensional PtSe 2. NANOPHOTONICS (BERLIN, GERMANY) 2024; 13:3457-3464. [PMID: 39634825 PMCID: PMC11501338 DOI: 10.1515/nanoph-2024-0107] [Citation(s) in RCA: 1] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 03/05/2024] [Accepted: 04/15/2024] [Indexed: 12/07/2024]
Abstract
Platinum diselenide (PtSe2), classified as a noble metal dichalcogenide, has garnered substantial interest owing to its layer-dependent band structure, remarkable air-stability, and high charge-carrier mobilities. These properties make it highly promising for a wide array of applications in next-generation electronic and optoelectronic devices, as well as sensors. Additionally, two-dimensional (2D) PtSe2 demonstrates significant potential as a saturable absorber due to its exceptional nonlinear optical response across an ultrabroad spectra range, presenting exciting opportunities in ultrafast and nonlinear photonics. In this work, we explore the second-order nonlinear optical characteristics of 2D PtSe2 by analyzing its second-harmonic generation (SHG) excited by a pulsed laser at 1064 nm. Our investigation unveils a layer-dependent SHG response in PtSe2, with prominent SHG intensity observed in few-layer PtSe2. The distinct six-fold polarization dependence pattern observed in the SHG intensity reflects the inherent threefold rotational symmetry inherent to the PtSe2 crystal structure. Remarkably, the SHG intensity of 4-layer PtSe2 surpasses that of mechanically exfoliated monolayer molybdenum disulfide (MoS2) by approximately two orders of magnitude (60-fold), underscoring its exceptional second-order nonlinear optical response. Combined with its ultrahigh air-stability, these distinctive nonlinear optical characteristics position two-dimensional PtSe2 as a promising candidate for ultrathin nonlinear nanophotonic devices.
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Affiliation(s)
- Lingrui Chu
- School of Physics, State Key Laboratory of Crystal Materials, Shandong University, Jinan250100, China
| | - Ziqi Li
- Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University, Singapore637371, Singapore
| | - Han Zhu
- School of Physics, State Key Laboratory of Crystal Materials, Shandong University, Jinan250100, China
| | - Hengyue Lv
- School of Physics, State Key Laboratory of Crystal Materials, Shandong University, Jinan250100, China
| | - Feng Chen
- School of Physics, State Key Laboratory of Crystal Materials, Shandong University, Jinan250100, China
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33
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Yu J, Mu H, Wang P, Li H, Yang Z, Ren J, Li Y, Mei L, Zhang J, Yu W, Cui N, Yuan J, Wu J, Lan S, Zhang G, Lin S. Anisotropic van der Waals Tellurene-Based Multifunctional, Polarization-Sensitive, In-Line Optical Device. ACS NANO 2024; 18:19099-19109. [PMID: 39001858 DOI: 10.1021/acsnano.4c03973] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 07/15/2024]
Abstract
Polarization plays a paramount role in scaling the optical network capacity. Anisotropic two-dimensional (2D) materials offer opportunities to exploit optical polarization-sensitive responses in various photonic and optoelectronic applications. However, the exploration of optical anisotropy in fiber in-line devices, critical for ultrafast pulse generation and modulation, remains limited. In this study, we present a fiber-integrated device based on a single-crystalline tellurene nanosheet. Benefiting from the chiral-chain crystal lattice and distinct optical dichroism of tellurene, multifunctional optical devices possessing diverse excellent properties can be achieved. By inserting the in-line device into a 1.5 μm fiber laser cavity, we generated both linearly polarized and dual-wavelength mode-locking pulses with a degree of polarization of 98% and exceptional long-term stability. Through a twisted configuration of two tellurene nanosheets, we realized an all-optical switching operation with a fast response. The multifunctional device also serves as a broadband photodetector. Notably, bipolar polarization encoding communication at 1550 nm can be achieved without any external voltage. The device's multifunctionality and stability in ambient environments established a promising prototype for integrating polarization as an additional physical dimension in fiber optical networks, encompassing diverse applications in light generation, modulation, and detection.
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Affiliation(s)
- Jing Yu
- Songshan Lake Materials Laboratory, Dongguan 523808, China
- Guangdong Provincial Key Laboratory of Nanophotonic Functional Materials and Devices, School of Information and Optoelectronic Science and Engineering, South China Normal University, Guangzhou 510006, China
| | - Haoran Mu
- Songshan Lake Materials Laboratory, Dongguan 523808, China
| | - Pu Wang
- Songshan Lake Materials Laboratory, Dongguan 523808, China
| | - Haozhe Li
- Songshan Lake Materials Laboratory, Dongguan 523808, China
| | - Zixin Yang
- College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha 410073, China
| | - Jing Ren
- Songshan Lake Materials Laboratory, Dongguan 523808, China
| | - Yang Li
- Songshan Lake Materials Laboratory, Dongguan 523808, China
| | - Luyao Mei
- Songshan Lake Materials Laboratory, Dongguan 523808, China
| | - Jingni Zhang
- Songshan Lake Materials Laboratory, Dongguan 523808, China
| | - Wenzhi Yu
- Songshan Lake Materials Laboratory, Dongguan 523808, China
| | - Nan Cui
- Songshan Lake Materials Laboratory, Dongguan 523808, China
| | - Jian Yuan
- State Key Laboratory of Applied Optics, Changchun Institute of Optics, Fine Mechanics and Physics, Chinese Academy of Sciences, Changchun 130033, China
| | - Jian Wu
- College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha 410073, China
| | - Sheng Lan
- Guangdong Provincial Key Laboratory of Nanophotonic Functional Materials and Devices, School of Information and Optoelectronic Science and Engineering, South China Normal University, Guangzhou 510006, China
| | - Guangyu Zhang
- Songshan Lake Materials Laboratory, Dongguan 523808, China
| | - Shenghuang Lin
- Songshan Lake Materials Laboratory, Dongguan 523808, China
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34
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Qin B, Ma C, Guo Q, Li X, Wei W, Ma C, Wang Q, Liu F, Zhao M, Xue G, Qi J, Wu M, Hong H, Du L, Zhao Q, Gao P, Wang X, Wang E, Zhang G, Liu C, Liu K. Interfacial epitaxy of multilayer rhombohedral transition-metal dichalcogenide single crystals. Science 2024; 385:99-104. [PMID: 38963849 DOI: 10.1126/science.ado6038] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 02/13/2024] [Accepted: 05/17/2024] [Indexed: 07/06/2024]
Abstract
Rhombohedral-stacked transition-metal dichalcogenides (3R-TMDs), which are distinct from their hexagonal counterparts, exhibit higher carrier mobility, sliding ferroelectricity, and coherently enhanced nonlinear optical responses. However, surface epitaxial growth of large multilayer 3R-TMD single crystals is difficult. We report an interfacial epitaxy methodology for their growth of several compositions, including molybdenum disulfide (MoS2), molybdenum diselenide, tungsten disulfide, tungsten diselenide, niobium disulfide, niobium diselenide, and molybdenum sulfoselenide. Feeding of metals and chalcogens continuously to the interface between a single-crystal Ni substrate and grown layers ensured consistent 3R stacking sequence and controlled thickness from a few to 15,000 layers. Comprehensive characterizations confirmed the large-scale uniformity, high crystallinity, and phase purity of these films. The as-grown 3R-MoS2 exhibited room-temperature mobilities up to 155 and 190 square centimeters per volt second for bi- and trilayers, respectively. Optical difference frequency generation with thick 3R-MoS2 showed markedly enhanced nonlinear response under a quasi-phase matching condition (five orders of magnitude greater than monolayers).
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Affiliation(s)
- Biao Qin
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing, China
- Key Laboratory of Quantum State Construction and Manipulation (Ministry of Education), Department of Physics, Renmin University of China, Beijing, China
| | - Chaojie Ma
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing, China
| | - Quanlin Guo
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing, China
| | - Xiuzhen Li
- Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing, China
| | - Wenya Wei
- Guangdong Basic Research Center of Excellence for Structure and Fundamental Interactions of Matter, Guangdong Provincial Key Laboratory of Quantum Engineering and Quantum Materials, School of Physics, South China Normal University, Guangzhou, China
| | - Chenjun Ma
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing, China
| | - Qinghe Wang
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing, China
| | - Fang Liu
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing, China
| | - Mengze Zhao
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing, China
| | - Guodong Xue
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing, China
| | - Jiajie Qi
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing, China
| | - Muhong Wu
- International Centre for Quantum Materials, Collaborative Innovation Centre of Quantum Matter, Peking University, Beijing, China
- Songshan Lake Materials Laboratory, Dongguan, China
- Interdisciplinary Institute of Light-Element Quantum Materials and Research Centre for Light-Element Advanced Materials, Peking University, Beijing, China
| | - Hao Hong
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing, China
- Interdisciplinary Institute of Light-Element Quantum Materials and Research Centre for Light-Element Advanced Materials, Peking University, Beijing, China
| | - Luojun Du
- Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing, China
| | - Qing Zhao
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing, China
| | - Peng Gao
- International Centre for Quantum Materials, Collaborative Innovation Centre of Quantum Matter, Peking University, Beijing, China
| | - Xinqiang Wang
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing, China
| | - Enge Wang
- International Centre for Quantum Materials, Collaborative Innovation Centre of Quantum Matter, Peking University, Beijing, China
- Songshan Lake Materials Laboratory, Dongguan, China
| | - Guangyu Zhang
- Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing, China
- Songshan Lake Materials Laboratory, Dongguan, China
| | - Can Liu
- Key Laboratory of Quantum State Construction and Manipulation (Ministry of Education), Department of Physics, Renmin University of China, Beijing, China
| | - Kaihui Liu
- State Key Laboratory for Mesoscopic Physics, Frontiers Science Centre for Nano-optoelectronics, School of Physics, Peking University, Beijing, China
- International Centre for Quantum Materials, Collaborative Innovation Centre of Quantum Matter, Peking University, Beijing, China
- Songshan Lake Materials Laboratory, Dongguan, China
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35
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Kourmoulakis G, Psilodimitrakopoulos S, Maragkakis GM, Mouchliadis L, Michail A, Christodoulides JA, Tripathi M, Dalton AB, Parthenios J, Papagelis K, Stratakis E, Kioseoglou G. Strain distribution in WS 2 monolayers detected through polarization-resolved second harmonic generation. Sci Rep 2024; 14:15159. [PMID: 38956262 PMCID: PMC11219737 DOI: 10.1038/s41598-024-66065-2] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 12/08/2023] [Accepted: 06/26/2024] [Indexed: 07/04/2024] Open
Abstract
Two-dimensional (2D) graphene and graphene-related materials (GRMs) show great promise for future electronic devices. GRMs exhibit distinct properties under the influence of the substrate that serves as support through uneven compression/ elongation of GRMs surface atoms. Strain in GRM monolayers is the most common feature that alters the interatomic distances and band structure, providing a new degree of freedom that allows regulation of their electronic properties and introducing the field of straintronics. Having an all-optical and minimally invasive detection tool that rapidly probes strain in large areas of GRM monolayers, would be of great importance in the research and development of novel 2D devices. Here, we use Polarization-resolved Second Harmonic Generation (P-SHG) optical imaging to identify strain distribution, induced in a single layer of WS2 placed on a pre-patterned Si/SiO2 substrate with cylindrical wells. By fitting the P-SHG data pixel-by-pixel, we produce spatially resolved images of the crystal armchair direction. In regions where the WS2 monolayer conforms to the pattern topography, a distinct cross-shaped pattern is evident in the armchair image owing to strain. The presence of strain in these regions is independently confirmed using a combination of atomic force microscopy and Raman mapping.
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Affiliation(s)
- George Kourmoulakis
- Institute of Electronic Structure and Laser, Foundation for Research and Technology - Hellas, 71110, Heraklion, Crete, Greece
- Department of Materials Science and Technology, University of Crete, 70013, Heraklion, Crete, Greece
| | - Sotiris Psilodimitrakopoulos
- Institute of Electronic Structure and Laser, Foundation for Research and Technology - Hellas, 71110, Heraklion, Crete, Greece.
| | - George Miltos Maragkakis
- Institute of Electronic Structure and Laser, Foundation for Research and Technology - Hellas, 71110, Heraklion, Crete, Greece
- Department of Physics, University of Crete, 70013, Heraklion, Crete, Greece
| | - Leonidas Mouchliadis
- Institute of Electronic Structure and Laser, Foundation for Research and Technology - Hellas, 71110, Heraklion, Crete, Greece
| | - Antonios Michail
- Department of Physics, University of Patras, 26504, Patras, Greece
- FORTH/ICE-HT, Stadiou Str Platani, 26504, Patras, Greece
| | | | - Manoj Tripathi
- Department of Physics and Astronomy, University of Sussex, Brighton, BN1 9RH, UK
| | - Alan B Dalton
- Department of Physics and Astronomy, University of Sussex, Brighton, BN1 9RH, UK
| | | | - Konstantinos Papagelis
- FORTH/ICE-HT, Stadiou Str Platani, 26504, Patras, Greece
- Department of Solid-State Physics, School of Physics, Aristotle University of Thessaloniki, 54124, Thessaloniki, Greece
| | - Emmanuel Stratakis
- Institute of Electronic Structure and Laser, Foundation for Research and Technology - Hellas, 71110, Heraklion, Crete, Greece.
- Department of Physics, University of Crete, 70013, Heraklion, Crete, Greece.
| | - George Kioseoglou
- Institute of Electronic Structure and Laser, Foundation for Research and Technology - Hellas, 71110, Heraklion, Crete, Greece.
- Department of Materials Science and Technology, University of Crete, 70013, Heraklion, Crete, Greece.
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36
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Wang JP, Chen X, Zhao Q, Fang Y, Liu Q, Fu J, Liu Y, Xu X, Zhang J, Zhen L, Xu CY, Huang F, Meixner AJ, Zhang D, Gou G, Li Y. Out-of-plane Emission Dipole of Second Harmonic Generation in Odd- and Even-layered vdWs Janus Nb 3SeI 7. ACS NANO 2024; 18:16274-16284. [PMID: 38867607 DOI: 10.1021/acsnano.4c02854] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/14/2024]
Abstract
Integration of atomically thin nonlinear optical (NLO) devices demands an out-of-plane (OP) emission dipole of second harmonic generation (SHG) to enhance the spontaneous emission for nanophotonics. However, the research on van der Waals (vdWs) materials with an OP emission dipole of SHG is still in its infancy. Here, by coupling back focal plane (BFP) imaging with numerical simulations and density functional theory (DFT) calculations, we demonstrate that vdWs Janus Nb3SeI7, ranging from bulk to the monolayer limit, exhibits a dominant OP emission dipole of SHG owing to the breaking of the OP symmetry. Explicitly, even-layered Nb3SeI7 with C6v symmetry is predicted to exhibit a pure OP emission dipole attributed to the only second-order susceptibility coefficient χzxx. Meanwhile, although odd-layered Nb3SeI7 with C3v symmetry has both OP and IP dipole components (χzxx and χyyy), the value of χzxx is 1 order of magnitude greater than that of χyyy, leading to an approximate OP emission dipole of SHG. Moreover, the crystal symmetry and OP emission dipole can be preserved under hydrostatic pressure, accompanied by the enhanced χzxx and the resulting 3-fold increase in SHG intensity. The reported stable OP dipole in 2D vdWs Nb3SeI7 can facilitate the rapid development of chip-integrated NLO devices.
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Affiliation(s)
- Jia-Peng Wang
- School of Materials Science and Engineering, Harbin Institute of Technology, Harbin 150001, China
| | - Xinfeng Chen
- Frontier Institute of Science and Technology & State Key Laboratory of Electrical Insulation and Power Equipment, Xi'an Jiaotong University, Xi' an 710049, China
| | - Qiyi Zhao
- School of Science, Xi'an University of Posts and Telecommunications, Xi'an 710199, China
| | - Yuqiang Fang
- State Key Laboratory of High-Performance Ceramics and Superfine Microstructure Shanghai Institute of Ceramics Chinese Academy of Sciences, Shanghai 200050, China
| | - Quan Liu
- Institute of Physical and Theoretical Chemistry, Eberhard Karls University Tübingen, Tübingen 72076, Germany
| | - Jierui Fu
- School of Materials Science and Engineering, Harbin Institute of Technology, Harbin 150001, China
| | - Yue Liu
- School of Materials Science and Engineering, Harbin Institute of Technology, Harbin 150001, China
| | - Xinlong Xu
- School of Physics, Northwest University, Xi'an 710069, China
| | - Jia Zhang
- MOE Key Laboratory of Micro-Systems and Micro-Structures Manufacturing, Harbin Institute of Technology, Harbin 150080, China
| | - Liang Zhen
- School of Materials Science and Engineering, Harbin Institute of Technology, Harbin 150001, China
- MOE Key Laboratory of Micro-Systems and Micro-Structures Manufacturing, Harbin Institute of Technology, Harbin 150080, China
| | - Cheng-Yan Xu
- School of Materials Science and Engineering, Harbin Institute of Technology, Harbin 150001, China
- MOE Key Laboratory of Micro-Systems and Micro-Structures Manufacturing, Harbin Institute of Technology, Harbin 150080, China
- Sauvage Laboratory for Smart Materials, School of Materials Science and Engineering, Harbin Institute of Technology Shenzhen, Shenzhen 518055, China
| | - Fuqiang Huang
- State Key Laboratory of High-Performance Ceramics and Superfine Microstructure Shanghai Institute of Ceramics Chinese Academy of Sciences, Shanghai 200050, China
| | - Alfred J Meixner
- Institute of Physical and Theoretical Chemistry, Eberhard Karls University Tübingen, Tübingen 72076, Germany
| | - Dai Zhang
- Institute of Physical and Theoretical Chemistry, Eberhard Karls University Tübingen, Tübingen 72076, Germany
| | - Gaoyang Gou
- Frontier Institute of Science and Technology & State Key Laboratory of Electrical Insulation and Power Equipment, Xi'an Jiaotong University, Xi' an 710049, China
| | - Yang Li
- School of Materials Science and Engineering, Harbin Institute of Technology, Harbin 150001, China
- MOE Key Laboratory of Micro-Systems and Micro-Structures Manufacturing, Harbin Institute of Technology, Harbin 150080, China
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37
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Lu P, Yan T, Huang J, Xing T, Liu H, Han Z, Xu X, Tao C. ITO-Induced Nonlinear Optical Response Enhancement of Titanium Nitride Thin Films. NANOMATERIALS (BASEL, SWITZERLAND) 2024; 14:1040. [PMID: 38921916 PMCID: PMC11206435 DOI: 10.3390/nano14121040] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 05/19/2024] [Revised: 06/10/2024] [Accepted: 06/14/2024] [Indexed: 06/27/2024]
Abstract
A series of TiN/ITO composite films with various thickness of ITO buffer layer were fabricated in this study. The enhancement of optical properties was realized in the composite thin films. The absorption spectra showed that absorption intensity in the near-infrared region was obviously enhanced with the increase of ITO thickness due to the coupling of surface plasma between TiN and ITO. The epsilon-near-zero wavelength of this composite can be tuned from 935 nm to 1895 nm by varying the thickness of ITO thin films. The nonlinear optical property investigated by Z-scan technique showed that the nonlinear absorption coefficient (β = 3.03 × 10-4 cm/W) for the composite was about 14.02 times greater than that of single-layer TiN films. The theoretical calculations performed by finite difference time domain were in good agreement with those of the experiments.
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Affiliation(s)
- Peng Lu
- Engineering Research Center of Optical Instrument and System, Ministry of Education and Shanghai Key Lab of Modern Optical System, University of Shanghai for Science and Technology, Shanghai 200093, China; (P.L.)
| | - Tingzhen Yan
- Department of Printing and Pack Aging Engineering, Shanghai Publishing and Printing College, No. 100 Shuifeng Road, Shanghai 200093, China;
| | - Jialei Huang
- Engineering Research Center of Optical Instrument and System, Ministry of Education and Shanghai Key Lab of Modern Optical System, University of Shanghai for Science and Technology, Shanghai 200093, China; (P.L.)
| | - Tian Xing
- Engineering Research Center of Optical Instrument and System, Ministry of Education and Shanghai Key Lab of Modern Optical System, University of Shanghai for Science and Technology, Shanghai 200093, China; (P.L.)
| | - Hao Liu
- Engineering Research Center of Optical Instrument and System, Ministry of Education and Shanghai Key Lab of Modern Optical System, University of Shanghai for Science and Technology, Shanghai 200093, China; (P.L.)
| | - Zhaoxia Han
- Engineering Research Center of Optical Instrument and System, Ministry of Education and Shanghai Key Lab of Modern Optical System, University of Shanghai for Science and Technology, Shanghai 200093, China; (P.L.)
| | - Xueke Xu
- Heng Mai Optics and Fine Mechanics (Hang Zhou) Co., Ltd., Hangzhou 311421, China
| | - Chunxian Tao
- Engineering Research Center of Optical Instrument and System, Ministry of Education and Shanghai Key Lab of Modern Optical System, University of Shanghai for Science and Technology, Shanghai 200093, China; (P.L.)
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38
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Chen D, Song Z, Yang C, Wei Y, Liu G, Meng L, Wu Q, Dang Y. Nonlinear Optical Effects of Hybrid Antimony(III) Halides Induced by Stereoactive 5s 2 Lone Pairs and Trimethylammonium Cations. Inorg Chem 2024; 63:10304-10311. [PMID: 38780359 DOI: 10.1021/acs.inorgchem.4c00980] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 05/25/2024]
Abstract
Organic-inorganic hybrid metal halides have unique optical and electronic properties, which are advantageous in the study of nonlinear optical materials. To investigate the effect of stereoactive lone pair electrons and the induction of organic cations on the structure of hybrid antimony(III) halides on nonlinear optics, we synthesize two noncentrosymmetric hybrid antimony(III)-based halide single crystals (TMA)3Sb2X9 (TMA = NH(CH3)3+, X = Cl, Br) by a room-temperature slow evaporation method, and their single-crystal structures, phase transition, X-ray photoelectron spectroscopy, and energy-band structure calculations are studied. More importantly, second-harmonic generation results of (TMA)3Sb2X9 (X = Cl, Br) are about 0.7 and 0.8 × KH2PO4(KDP), respectively. Interestingly, (TMA)3Sb2Cl9 single crystals undergo a reversible structural transition from Pc (No. 7) at room temperature to P21/c (No. 14) at 400 K, while the (TMA)3Sb2Br9 single crystals belong to the noncentrosymmetric space group R3c (No. 161), which clarifies the previous results. This work not only deepens the understanding of the role in lone pair electrons and organic cations in the structural induction in antimony-based halide perovskite materials but also provides guidance for subsequent nonlinear optical explorations.
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Affiliation(s)
- Danping Chen
- School of Physics and Physical Engineering, Qufu Normal University, Qufu 273165, P. R. China
| | - Zhexin Song
- School of Physics and Physical Engineering, Qufu Normal University, Qufu 273165, P. R. China
| | - Can Yang
- State Key Laboratory of New Textile Materials and Advanced Processing Technologies, Wuhan Textile University, Wuhan 430200, P. R. China
| | - Yaoyao Wei
- School of Chemistry and Chemical Engineering, Linyi University, Linyi 276000, P. R. China
| | - Guokui Liu
- School of Chemistry and Chemical Engineering, Linyi University, Linyi 276000, P. R. China
| | - Lingqiang Meng
- School of Advanced Materials, Peking University Shenzhen Graduate School, Peking University, Shenzhen 518055, P. R. China
| | - Qi Wu
- State Key Laboratory of New Textile Materials and Advanced Processing Technologies, Wuhan Textile University, Wuhan 430200, P. R. China
| | - Yangyang Dang
- School of Physics and Physical Engineering, Qufu Normal University, Qufu 273165, P. R. China
- State Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, P. R. China
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39
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Chen W, Zhu S, Duan R, Wang C, Wang F, Wu Y, Dai M, Cui J, Chae SH, Li Z, Ma X, Wang Q, Liu Z, Wang QJ. Extraordinary Enhancement of Nonlinear Optical Interaction in NbOBr 2 Microcavities. ADVANCED MATERIALS (DEERFIELD BEACH, FLA.) 2024; 36:e2400858. [PMID: 38631028 DOI: 10.1002/adma.202400858] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/17/2024] [Revised: 04/04/2024] [Indexed: 04/19/2024]
Abstract
2D materials are burgeoning as promising candidates for investigating nonlinear optical effects due to high nonlinear susceptibilities, broadband optical response, and tunable nonlinearity. However, most 2D materials suffer from poor nonlinear conversion efficiencies, resulting from reduced light-matter interactions and lack of phase matching at atomic thicknesses. Herein, a new 2D nonlinear material, niobium oxide dibromide (NbOBr2) is reported, featuring strong and anisotropic optical nonlinearities with scalable nonlinear intensity. Furthermore, Fabry-Pérot (F-P) microcavities are constructed by coupling NbOBr2 with air holes in silicon. Remarkable enhancement factors of ≈630 times in second harmonic generation (SHG) and 210 times in third harmonic generation (THG) are achieved on cavity at the resonance wavelength of 1500 nm. Notably, the cavity enhancement effect exhibits strong anisotropic feature tunable with pump wavelength, owing to the robust optical birefringence of NbOBr2. The ratio of the enhancement factor along the b- and c-axis of NbOBr2 reaches 2.43 and 5.27 for SHG and THG at 1500 nm pump, respectively, which leads to an extraordinarily high SHG anisotropic ratio of 17.82 and a 10° rotation of THG polarization. The research presents a feasible and practical strategy for developing high-efficiency and low-power-pumped on-chip nonlinear optical devices with tunable anisotropy.
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Affiliation(s)
- Wenduo Chen
- School of Electrical and Electronic Engineering, Nanyang Technological University, Singapore, 639798, Singapore
| | - Song Zhu
- School of Electrical and Electronic Engineering, Nanyang Technological University, Singapore, 639798, Singapore
| | - Ruihuan Duan
- School of Materials Science and Engineering, Nanyang Technological University, Singapore, 639798, Singapore
| | - Chongwu Wang
- School of Electrical and Electronic Engineering, Nanyang Technological University, Singapore, 639798, Singapore
| | - Fakun Wang
- School of Electrical and Electronic Engineering, Nanyang Technological University, Singapore, 639798, Singapore
| | - Yao Wu
- School of Materials Science and Engineering, Nanyang Technological University, Singapore, 639798, Singapore
| | - Mingjin Dai
- School of Electrical and Electronic Engineering, Nanyang Technological University, Singapore, 639798, Singapore
| | - Jieyuan Cui
- School of Electrical and Electronic Engineering, Nanyang Technological University, Singapore, 639798, Singapore
| | - Sang Hoon Chae
- School of Electrical and Electronic Engineering, Nanyang Technological University, Singapore, 639798, Singapore
| | - Zhipeng Li
- Institute of Materials Research and Engineering (IMRE), Agency for Science, Technology and Research (A*STAR), 2 Fusionopolis Way, Innovis, #08-03, Singapore, 138634, Singapore
| | - Xuezhi Ma
- Institute of Materials Research and Engineering (IMRE), Agency for Science, Technology and Research (A*STAR), 2 Fusionopolis Way, Innovis, #08-03, Singapore, 138634, Singapore
| | - Qian Wang
- Institute of Materials Research and Engineering (IMRE), Agency for Science, Technology and Research (A*STAR), 2 Fusionopolis Way, Innovis, #08-03, Singapore, 138634, Singapore
| | - Zheng Liu
- School of Electrical and Electronic Engineering, Nanyang Technological University, Singapore, 639798, Singapore
- School of Materials Science and Engineering, Nanyang Technological University, Singapore, 639798, Singapore
| | - Qi Jie Wang
- School of Electrical and Electronic Engineering, Nanyang Technological University, Singapore, 639798, Singapore
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40
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Zhu S, Duan R, Xu X, Sun F, Chen W, Wang F, Li S, Ye M, Zhou X, Cheng J, Wu Y, Liang H, Kono J, Li X, Liu Z, Wang QJ. Strong nonlinear optical processes with extraordinary polarization anisotropy in inversion-symmetry broken two-dimensional PdPSe. LIGHT, SCIENCE & APPLICATIONS 2024; 13:119. [PMID: 38802363 PMCID: PMC11130276 DOI: 10.1038/s41377-024-01474-6] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/14/2024] [Revised: 05/03/2024] [Accepted: 05/09/2024] [Indexed: 05/29/2024]
Abstract
Nonlinear optical activities, especially second harmonic generation (SHG), are key phenomena in inversion-symmetry-broken two-dimensional (2D) transition metal dichalcogenides (TMDCs). On the other hand, anisotropic nonlinear optical processes are important for unique applications in nano-nonlinear photonic devices with polarization functions, having become one of focused research topics in the field of nonlinear photonics. However, the strong nonlinearity and strong optical anisotropy do not exist simultaneously in common 2D materials. Here, we demonstrate strong second-order and third-order susceptibilities of 64 pm/V and 6.2×10-19 m2/V2, respectively, in the even-layer PdPSe, which has not been discovered in other common TMDCs (e.g., MoS2). Strikingly, it also simultaneously exhibited strong SHG anisotropy with an anisotropic ratio of ~45, which is the largest reported among all 2D materials to date, to the best of our knowledge. In addition, the SHG anisotropy ratio can be harnessed from 0.12 to 45 (375 times) by varying the excitation wavelength due to the dispersion ofχ ( 2 ) values. As an illustrative example, we further demonstrate polarized SHG imaging for potential applications in crystal orientation identification and polarization-dependent spatial encoding. These findings in 2D PdPSe are promising for nonlinear nanophotonic and optoelectronic applications.
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Affiliation(s)
- Song Zhu
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798, Singapore, Singapore
| | - Ruihuan Duan
- School of Material Science and Engineering, Nanyang Technological University, 639798, Singapore, Singapore
- CINTRA CNRS/NTU/THALES, UMI 3288, Research Techno Plaza, Nanyang Technological University, 637371, Singapore, Singapore
| | - Xiaodong Xu
- School of Materials Science and Engineering, Harbin Institute of Technology, 150001, Harbin, China
| | - Fangyuan Sun
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798, Singapore, Singapore
| | - Wenduo Chen
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798, Singapore, Singapore
| | - Fakun Wang
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798, Singapore, Singapore
| | - Siyuan Li
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798, Singapore, Singapore
| | - Ming Ye
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798, Singapore, Singapore
| | - Xin Zhou
- Department of Chemistry, National University of Singapore, 117543, Singapore, Singapore
| | - Jinluo Cheng
- GPL Photonics Lab, State Key Laboratory of Applied Optics, Changchun Institute of Optics, Fine Mechanics and Physics, Chinese Academy of Sciences, 130033, Changchun, China
| | - Yao Wu
- School of Material Science and Engineering, Nanyang Technological University, 639798, Singapore, Singapore
| | - Houkun Liang
- School of Electronics and Information Engineering, Sichuan University, 610064, Chengdu, Sichuan, China
| | - Junichiro Kono
- School of Physical and Mathematical Sciences, Nanyang Technological University, 637371, Singapore, Singapore
- Departments of Electrical and Computer Engineering, Physics and Astronomy, and Materials Science and NanoEngineering, Rice University, Houston, TX, USA
| | - Xingji Li
- School of Materials Science and Engineering, Harbin Institute of Technology, 150001, Harbin, China.
| | - Zheng Liu
- School of Material Science and Engineering, Nanyang Technological University, 639798, Singapore, Singapore.
- CINTRA CNRS/NTU/THALES, UMI 3288, Research Techno Plaza, Nanyang Technological University, 637371, Singapore, Singapore.
| | - Qi Jie Wang
- School of Electrical and Electronic Engineering, Nanyang Technological University, 639798, Singapore, Singapore.
- CINTRA CNRS/NTU/THALES, UMI 3288, Research Techno Plaza, Nanyang Technological University, 637371, Singapore, Singapore.
- School of Physical and Mathematical Sciences, Nanyang Technological University, 637371, Singapore, Singapore.
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41
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Younus K, Zhou Y, Zhu M, Xu D, Guo X, Ahmed A, Ouyang F, Huang H, Xiao S, Chen Z, He J. Observation of Anisotropic Second Harmonic Generation in Two-Dimensional Niobium Diselenide. J Phys Chem Lett 2024; 15:4992-4999. [PMID: 38695534 DOI: 10.1021/acs.jpclett.4c00923] [Citation(s) in RCA: 1] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/15/2025]
Abstract
The intrinsic anisotropy of NbSe2 provides a favorable prerequisite of second harmonic generation (SHG) and rich possibilities for tailoring its nonlinear optical (NLO) properties. Here we report the highly efficient SHG of mechanically exfoliated NbSe2 flakes. The nonlinear optical response changes with excitation wavelengths, layer thicknesses, and polarizations of the excitation laser. The anisotropic SHG response further exhibits the intrinsic non-centrosymmetric crystal structure and could effectively assign the crystalline orientation of NbSe2 flakes. Interestingly, although NbSe2 flakes with tens of nanometers thickness experience attenuations in SHG performance, more efficient SHG anisotropy ratios were obtained, which are around 4 times higher than that of the 5-layer counterpart. The determined second-order nonlinearities of NbSe2 flakes (monolayer: ∼1.0 × 103 pm/V; 3-layer: ∼73 pm/V) are comparable to those of the commonly reported two-dimensional materials (e.g., MoS2, WSe2, graphene) with the same number of layers and much higher than those of commercial nonlinear optical crystals.
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Affiliation(s)
- Khansa Younus
- Hunan Key Laboratory of Nanophotonics and Devices, School of Physics, Central South University, 932 South Lushan Road, Changsha, Hunan 410083, P. R. China
| | - Yu Zhou
- Hunan Key Laboratory of Nanophotonics and Devices, School of Physics, Central South University, 932 South Lushan Road, Changsha, Hunan 410083, P. R. China
| | - Menglong Zhu
- Department of Applied Physics, School of Microelectronics and Physics, Hunan University of Technology and Business, Changsha 410205, China
| | - Defeng Xu
- Hunan Key Laboratory of Nanophotonics and Devices, School of Physics, Central South University, 932 South Lushan Road, Changsha, Hunan 410083, P. R. China
| | - Xiao Guo
- Hunan Key Laboratory of Nanophotonics and Devices, School of Physics, Central South University, 932 South Lushan Road, Changsha, Hunan 410083, P. R. China
| | - Asad Ahmed
- Hunan Key Laboratory of Nanophotonics and Devices, School of Physics, Central South University, 932 South Lushan Road, Changsha, Hunan 410083, P. R. China
| | - Fangping Ouyang
- Hunan Key Laboratory of Nanophotonics and Devices, School of Physics, Central South University, 932 South Lushan Road, Changsha, Hunan 410083, P. R. China
- School of Physics and Technology, State Key Laboratory of Chemistry and Utilization of Carbon Based Energy Resources, Xinjiang University, Urumqi 830046, People's Republic of China
| | - Han Huang
- Hunan Key Laboratory of Nanophotonics and Devices, School of Physics, Central South University, 932 South Lushan Road, Changsha, Hunan 410083, P. R. China
| | - Si Xiao
- Hunan Key Laboratory of Nanophotonics and Devices, School of Physics, Central South University, 932 South Lushan Road, Changsha, Hunan 410083, P. R. China
| | - Zhihui Chen
- Hunan Key Laboratory of Nanophotonics and Devices, School of Physics, Central South University, 932 South Lushan Road, Changsha, Hunan 410083, P. R. China
| | - Jun He
- Hunan Key Laboratory of Nanophotonics and Devices, School of Physics, Central South University, 932 South Lushan Road, Changsha, Hunan 410083, P. R. China
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42
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Yang Z, Zhang T, Dai J, Xu K. Tunable-bias based optical neural network for reinforcement learning in path planning. OPTICS EXPRESS 2024; 32:18099-18112. [PMID: 38858974 DOI: 10.1364/oe.516173] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 12/15/2023] [Accepted: 03/12/2024] [Indexed: 06/12/2024]
Abstract
Owing to the high integration, reconfiguration and strong robustness, Mach-Zehnder interferometers (MZIs) based optical neural networks (ONNs) have been widely considered. However, there are few works adding bias, which is important for neural networks, into the ONNs and systematically studying its effect. In this article, we propose a tunable-bias based optical neural network (TBONN) with one unitary matrix layer, which can improve the utilization rate of the MZIs, increase the trainable weights of the network and has more powerful representational capacity than traditional ONNs. By systematically studying its underlying mechanism and characteristics, we demonstrate that TBONN can achieve higher performance by adding more optical biases to the same side beside the inputted signals. For the two-dimensional dataset, the average prediction accuracy of TBONN with 2 biases (97.1%) is 5% higher than that of TBONN with 0 biases (92.1%). Additionally, utilizing TBONN, we propose a novel optical deep Q network (ODQN) algorithm to complete path planning tasks. By implementing simulated experiments, our ODQN shows competitive performance compared with the conventional deep Q network, but accelerates the computation speed by 2.5 times and 4.5 times for 2D and 3D grid worlds, respectively. Further, a more noticeable acceleration will be obtained when applying TBONN to more complex tasks. Also, we demonstrate the strong robustness of TBONN and the imprecision elimination method by using on-chip training.
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43
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Xiong H, Nie X, Zhao L, Deng S. Engineering Symmetry Breaking in Twisted MoS 2-MoSe 2 Heterostructures for Optimal Thermoelectric Performance. ACS APPLIED MATERIALS & INTERFACES 2024. [PMID: 38709893 DOI: 10.1021/acsami.4c03767] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/08/2024]
Abstract
Engineering symmetry breaking in thermoelectric materials holds promise for achieving an optimal thermoelectric efficiency. van der Waals (vdW) layered transition metal dichalcogenides (TMDCs) provide critical opportunities for manipulating the intrinsic symmetry through in-plane symmetry breaking interlayer twists and out-of-plane symmetry breaking heterostructures. Herein, the symmetry-dependent thermoelectric properties of MoS2 and MoSe2 obtained via first-principles calculations are reported, yielding an advanced ZT of 2.96 at 700 K. The underlying mechanisms reveal that the in-plane symmetry breaking results in a lowest thermal conductivity of 1.96 W·m-1·K-1. Additionally, the electric properties can be significantly modulated through band flattening and bandgap alteration, stemming directly from the modified interlayer electronic coupling strength owing to spatial repulsion effects. In addition, out-of-plane symmetry breaking induces band splitting, leading to a decrease in the degeneracy and complex band structures. Consequently, the power factor experiences a notable enhancement from ∼1.32 to 1.71 × 10-2 W·m-1·K-2, which is attributed to the intricate spatial configuration of charge densities and the resulting intensified intralayer electronic coupling. Upon simultaneous implementation of in-plane and out-of-plane symmetry breaking, the TMDCs exhibit an indirect bandgap to direct bandgap transition compared to the pristine structure. This work demonstrates an avenue for optimizing thermoelectric performance of TMDCs through the implementation of symmetry breaking.
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Affiliation(s)
- Hanping Xiong
- State Key Laboratory of Engines, Tianjin University, Tianjin 300350, China
| | - Xianhua Nie
- State Key Laboratory of Engines, Tianjin University, Tianjin 300350, China
| | - Li Zhao
- State Key Laboratory of Engines, Tianjin University, Tianjin 300350, China
| | - Shuai Deng
- State Key Laboratory of Engines, Tianjin University, Tianjin 300350, China
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44
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Song S, Rahaman M, Jariwala D. Can 2D Semiconductors Be Game-Changers for Nanoelectronics and Photonics? ACS NANO 2024; 18:10955-10978. [PMID: 38625032 DOI: 10.1021/acsnano.3c12938] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 04/17/2024]
Abstract
2D semiconductors have interesting physical and chemical attributes that have led them to become one of the most intensely investigated semiconductor families in recent history. They may play a crucial role in the next technological revolution in electronics as well as optoelectronics or photonics. In this Perspective, we explore the fundamental principles and significant advancements in electronic and photonic devices comprising 2D semiconductors. We focus on strategies aimed at enhancing the performance of conventional devices and exploiting important properties of 2D semiconductors that allow fundamentally interesting device functionalities for future applications. Approaches for the realization of emerging logic transistors and memory devices as well as photovoltaics, photodetectors, electro-optical modulators, and nonlinear optics based on 2D semiconductors are discussed. We also provide a forward-looking perspective on critical remaining challenges and opportunities for basic science and technology level applications of 2D semiconductors.
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Affiliation(s)
- Seunguk Song
- Department of Electrical and Systems Engineering, University of Pennsylvania, Philadelphia, Pennsylvania 19104, United States
| | - Mahfujur Rahaman
- Department of Electrical and Systems Engineering, University of Pennsylvania, Philadelphia, Pennsylvania 19104, United States
| | - Deep Jariwala
- Department of Electrical and Systems Engineering, University of Pennsylvania, Philadelphia, Pennsylvania 19104, United States
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45
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Fu Y, Liu Z, Yue S, Zhang K, Wang R, Zhang Z. Optical Second Harmonic Generation of Low-Dimensional Semiconductor Materials. NANOMATERIALS (BASEL, SWITZERLAND) 2024; 14:662. [PMID: 38668156 PMCID: PMC11054873 DOI: 10.3390/nano14080662] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 02/24/2024] [Revised: 04/02/2024] [Accepted: 04/07/2024] [Indexed: 04/29/2024]
Abstract
In recent years, the phenomenon of optical second harmonic generation (SHG) has attracted significant attention as a pivotal nonlinear optical effect in research. Notably, in low-dimensional materials (LDMs), SHG detection has become an instrumental tool for elucidating nonlinear optical properties due to their pronounced second-order susceptibility and distinct electronic structure. This review offers an exhaustive overview of the generation process and experimental configurations for SHG in such materials. It underscores the latest advancements in harnessing SHG as a sensitive probe for investigating the nonlinear optical attributes of these materials, with a particular focus on its pivotal role in unveiling electronic structures, bandgap characteristics, and crystal symmetry. By analyzing SHG signals, researchers can glean invaluable insights into the microscopic properties of these materials. Furthermore, this paper delves into the applications of optical SHG in imaging and time-resolved experiments. Finally, future directions and challenges toward the improvement in the NLO in LDMs are discussed to provide an outlook in this rapidly developing field, offering crucial perspectives for the design and optimization of pertinent devices.
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Affiliation(s)
- Yue Fu
- Microelectronics Instruments and Equipment R&D Center, Institute of Microelectronics, Chinese Academy of Sciences, 3 Beitucheng West Road, Beijing 100029, China; (Y.F.); (Z.L.); (S.Y.); (K.Z.)
| | - Zhengyan Liu
- Microelectronics Instruments and Equipment R&D Center, Institute of Microelectronics, Chinese Academy of Sciences, 3 Beitucheng West Road, Beijing 100029, China; (Y.F.); (Z.L.); (S.Y.); (K.Z.)
- School of Integrated Circuits, University of Chinese Academy of Sciences, No. 19(A) Yuquan Road, Beijing 100049, China
| | - Song Yue
- Microelectronics Instruments and Equipment R&D Center, Institute of Microelectronics, Chinese Academy of Sciences, 3 Beitucheng West Road, Beijing 100029, China; (Y.F.); (Z.L.); (S.Y.); (K.Z.)
- School of Integrated Circuits, University of Chinese Academy of Sciences, No. 19(A) Yuquan Road, Beijing 100049, China
| | - Kunpeng Zhang
- Microelectronics Instruments and Equipment R&D Center, Institute of Microelectronics, Chinese Academy of Sciences, 3 Beitucheng West Road, Beijing 100029, China; (Y.F.); (Z.L.); (S.Y.); (K.Z.)
| | - Ran Wang
- Microelectronics Instruments and Equipment R&D Center, Institute of Microelectronics, Chinese Academy of Sciences, 3 Beitucheng West Road, Beijing 100029, China; (Y.F.); (Z.L.); (S.Y.); (K.Z.)
- School of Integrated Circuits, University of Chinese Academy of Sciences, No. 19(A) Yuquan Road, Beijing 100049, China
| | - Zichen Zhang
- Microelectronics Instruments and Equipment R&D Center, Institute of Microelectronics, Chinese Academy of Sciences, 3 Beitucheng West Road, Beijing 100029, China; (Y.F.); (Z.L.); (S.Y.); (K.Z.)
- School of Integrated Circuits, University of Chinese Academy of Sciences, No. 19(A) Yuquan Road, Beijing 100049, China
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46
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Bykov AY, Deng J, Li G, Zayats AV. Time-Dependent Ultrafast Quadratic Nonlinearity in an Epsilon-Near-Zero Platform. NANO LETTERS 2024; 24:3744-3749. [PMID: 38483127 PMCID: PMC10979426 DOI: 10.1021/acs.nanolett.4c00282] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/18/2024] [Revised: 02/22/2024] [Accepted: 03/06/2024] [Indexed: 03/28/2024]
Abstract
Ultrafast nonlinearity, which results in modulation of the linear optical response, is a basis for the development of time-varying media, in particular those operating in the epsilon-near-zero (ENZ) regime. Here, we demonstrate that the intraband excitation of hot electrons in the ENZ film results in a second-harmonic resonance shift of ∼10 THz (40 nm) and second-harmonic generation (SHG) intensity changes of >100% with only minor (<1%) changes in linear transmission. The modulation is 10-fold enhanced by a plasmonic metasurface coupled to a film, allowing for ultrafast modulation of circularly polarized SHG. The effect is described by the plasma frequency renormalization in the ENZ material and the modification of the electron damping, with a possible influence of the hot-electron dynamics on the quadratic susceptibility. The results elucidate the nature of the second-order nonlinearity in ENZ materials and pave the way to the rational engineering of active nonlinear metamaterials and metasurfaces for time-varying applications.
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Affiliation(s)
- Anton Yu. Bykov
- Department
of Physics and London Centre for Nanotechnology, King’s College London, London WS2R 2LS, U.K.
| | - Junhong Deng
- Shenzhen
Institute for Quantum Science and Engineering, Southern University of Science and Technology, Shenzhen 518055, China
| | - Guixin Li
- Department
of Materials Science and Engineering, Southern
University of Science and Technology, Shenzhen 518055, China
| | - Anatoly V. Zayats
- Department
of Physics and London Centre for Nanotechnology, King’s College London, London WS2R 2LS, U.K.
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47
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Wang Y, Wang G, Wang Y, Zhou L, Kang J, Zheng W, Xiao S, Xing G, He J. Two-Dimensional Molybdenum Boride (MBene) Mo 4/3B 2T x with Broadband and Termination-Dependent Ultrafast Nonlinear Optical Response. J Phys Chem Lett 2024:3461-3469. [PMID: 38512334 DOI: 10.1021/acs.jpclett.3c03493] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 03/22/2024]
Abstract
Two-dimensional molybdenum borides (MBenes) comprise a new class of 2D transition metal borides that exhibit potential photonics applications. Recently, the synthesis of individual single-layer Mo4/3B2Tx (T = O, F, OH) MBene sheets has been realized, which attracted considerable attention in optoelectronics. However, there is still a lack of understanding and regulation of the photophysical processes of Mo4/3B2Tx MBene. Here, we demonstrate that Mo4/3B2Tx MBene exhibits a surface termination-dependent electronic structure, carrier dynamics, and nonlinear optical response over a wide wavelength range (500-1550 nm). As prepared 2D Mo4/3B2F2 MBene possesses a semimetal material property that exhibits a shorter intraband scattering process (<100 ps) and a considerable nonlinear optical response at a broadband cover optical communication C band at 1550 nm. These thrilling results are confirmed theoretically and experimentally. The analysis of these results adds to the regulating and understanding of the basic photophysical processes, which is anticipated to be beneficial for the further design of MBene-based photonics and nanoelectronics devices.
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Affiliation(s)
- Yiduo Wang
- Hunan Key Laboratory of Nanophotonics and Devices, School of Physics and Electronics, Central South University, Changsha 410083, P.R.China
- Hunan Key Laboratory for Super-microstructure and Ultrafast Process, School of Physics and Electronics, Central South University, 932 South Lushan Road, Changsha, Hunan 410083, P.R.China
| | - Gang Wang
- Joint Key Laboratory of the Ministry of Education, Institute of Applied Physics and Materials Engineering, University of Macau, Avenida da Universidade, Taipa, Macao SAR 999078, China
| | - Yingwei Wang
- Hunan Key Laboratory of Nanophotonics and Devices, School of Physics and Electronics, Central South University, Changsha 410083, P.R.China
- Hunan Key Laboratory for Super-microstructure and Ultrafast Process, School of Physics and Electronics, Central South University, 932 South Lushan Road, Changsha, Hunan 410083, P.R.China
| | - Li Zhou
- Hunan Key Laboratory of Nanophotonics and Devices, School of Physics and Electronics, Central South University, Changsha 410083, P.R.China
- Hunan Key Laboratory for Super-microstructure and Ultrafast Process, School of Physics and Electronics, Central South University, 932 South Lushan Road, Changsha, Hunan 410083, P.R.China
| | - Jianlong Kang
- Hunan Key Laboratory of Nanophotonics and Devices, School of Physics and Electronics, Central South University, Changsha 410083, P.R.China
- Hunan Key Laboratory for Super-microstructure and Ultrafast Process, School of Physics and Electronics, Central South University, 932 South Lushan Road, Changsha, Hunan 410083, P.R.China
| | - Wanxin Zheng
- Hunan Key Laboratory of Nanophotonics and Devices, School of Physics and Electronics, Central South University, Changsha 410083, P.R.China
- Hunan Key Laboratory for Super-microstructure and Ultrafast Process, School of Physics and Electronics, Central South University, 932 South Lushan Road, Changsha, Hunan 410083, P.R.China
| | - Si Xiao
- Hunan Key Laboratory of Nanophotonics and Devices, School of Physics and Electronics, Central South University, Changsha 410083, P.R.China
- Hunan Key Laboratory for Super-microstructure and Ultrafast Process, School of Physics and Electronics, Central South University, 932 South Lushan Road, Changsha, Hunan 410083, P.R.China
| | - Guichuan Xing
- Joint Key Laboratory of the Ministry of Education, Institute of Applied Physics and Materials Engineering, University of Macau, Avenida da Universidade, Taipa, Macao SAR 999078, China
| | - Jun He
- Hunan Key Laboratory of Nanophotonics and Devices, School of Physics and Electronics, Central South University, Changsha 410083, P.R.China
- Hunan Key Laboratory for Super-microstructure and Ultrafast Process, School of Physics and Electronics, Central South University, 932 South Lushan Road, Changsha, Hunan 410083, P.R.China
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48
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Wasem Klein F, Huntzinger JR, Astié V, Voiry D, Parret R, Makhlouf H, Juillaguet S, Decams JM, Contreras S, Landois P, Zahab AA, Sauvajol JL, Paillet M. Determining by Raman spectroscopy the average thickness and N-layer-specific surface coverages of MoS 2 thin films with domains much smaller than the laser spot size. BEILSTEIN JOURNAL OF NANOTECHNOLOGY 2024; 15:279-296. [PMID: 38476324 PMCID: PMC10928926 DOI: 10.3762/bjnano.15.26] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 11/13/2023] [Accepted: 02/20/2024] [Indexed: 03/14/2024]
Abstract
Raman spectroscopy is a widely used technique to characterize nanomaterials because of its convenience, non-destructiveness, and sensitivity to materials change. The primary purpose of this work is to determine via Raman spectroscopy the average thickness of MoS2 thin films synthesized by direct liquid injection pulsed-pressure chemical vapor deposition (DLI-PP-CVD). Such samples are constituted of nanoflakes (with a lateral size of typically 50 nm, i.e., well below the laser spot size), with possibly a distribution of thicknesses and twist angles between stacked layers. As an essential preliminary, we first reassess the applicability of different Raman criteria to determine the thicknesses (or layer number, N) of MoS2 flakes from measurements performed on reference samples, namely well-characterized mechanically exfoliated or standard chemical vapor deposition MoS2 large flakes deposited on 90 ± 6 nm SiO2 on Si substrates. Then, we discuss the applicability of the same criteria for significantly different DLI-PP-CVD MoS2 samples with average thicknesses ranging from sub-monolayer up to three layers. Finally, an original procedure based on the measurement of the intensity of the layer breathing modes is proposed to evaluate the surface coverage for each N (i.e., the ratio between the surface covered by exactly N layers and the total surface) in DLI-PP-CVD MoS2 samples.
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Affiliation(s)
- Felipe Wasem Klein
- Laboratoire Charles Coulomb, Université de Montpellier, CNRS, F-34095, Montpellier, France
| | - Jean-Roch Huntzinger
- Laboratoire Charles Coulomb, Université de Montpellier, CNRS, F-34095, Montpellier, France
| | - Vincent Astié
- Annealsys, 139 Rue des Walkyries, 34000 Montpellier, France
| | - Damien Voiry
- Institut Européen des Membranes, IEM, UMR 5635, Université Montpellier, ENSCM, CNRS, Montpellier, France
| | - Romain Parret
- Aix Marseille Université, CNRS, CINAM, UMR 7325, Campus de Luminy, 13288, Marseille, France
| | - Houssine Makhlouf
- Laboratoire Charles Coulomb, Université de Montpellier, CNRS, F-34095, Montpellier, France
| | - Sandrine Juillaguet
- Laboratoire Charles Coulomb, Université de Montpellier, CNRS, F-34095, Montpellier, France
| | | | - Sylvie Contreras
- Laboratoire Charles Coulomb, Université de Montpellier, CNRS, F-34095, Montpellier, France
| | - Périne Landois
- Laboratoire Charles Coulomb, Université de Montpellier, CNRS, F-34095, Montpellier, France
| | - Ahmed-Azmi Zahab
- Laboratoire Charles Coulomb, Université de Montpellier, CNRS, F-34095, Montpellier, France
| | - Jean-Louis Sauvajol
- Laboratoire Charles Coulomb, Université de Montpellier, CNRS, F-34095, Montpellier, France
| | - Matthieu Paillet
- Laboratoire Charles Coulomb, Université de Montpellier, CNRS, F-34095, Montpellier, France
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49
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Li N, Zhang N, Wang J, Sun M. Charge transfer excitons and directional fluorescence of in-plane lateral MoSe 2-WSe 2 heterostructures. Phys Chem Chem Phys 2024; 26:8200-8209. [PMID: 38381067 DOI: 10.1039/d3cp04761j] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 02/22/2024]
Abstract
In this article, the linear and nonlinear optical properties of in-plane lateral MoSe2-WSe2 heterostructures are theoretically investigated. The polarization-dependent strongest optical absorption in one-photon absorption occurs in charge transfer excited states, where electrons transfer from WSe2 to MoSe2. This phenomenon is supported by the LUMO (lowest unoccupied molecular orbital) and HUMO (highest occupied molecular orbital) imaging obtained through scanning tunneling microscopy. The charge difference density and transition density matrix are used to interpret the electronic transitions, and these interpretations rely on the concept of transition density. The optical properties of two-photon absorption in its nonlinear optical process are significantly different from the excitation in one-photon absorption, where the strongest optical absorption is contributed from direct transition from the ground state to the final state without going through an intermediate excited state, due to the very large difference of permanent dipole moments between the excited and ground states. Our results also reveal directional fluorescence and physical mechanism of in-plane lateral MoSe2-WSe2 heterostructures. Our work can provide insights into the physical mechanism of the optical properties of in-plane lateral MoSe2-WSe2 heterostructures.
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Affiliation(s)
- Ning Li
- School of Mathematics and Physics, University of Science and Technology Beijing, Beijing 100083, China.
| | - Na Zhang
- College of Science, Liaoning Petrochemical University, Fushun 113001, China
| | - Jingang Wang
- College of Science, Liaoning Petrochemical University, Fushun 113001, China
| | - Mengtao Sun
- School of Mathematics and Physics, University of Science and Technology Beijing, Beijing 100083, China.
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50
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Niu X, Yuan M, Zhao R, Liu Y, Wang L, Pang Z, Wan S, Zhao H, Li H, Wang K. pH-Tuned Enantioselectivity Reversal in a Defective Chiral Metal Organic Framework. ACS Sens 2024; 9:923-931. [PMID: 38335470 DOI: 10.1021/acssensors.3c02330] [Citation(s) in RCA: 5] [Impact Index Per Article: 5.0] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 02/12/2024]
Abstract
The introduction of chirality into easy-scalable metal-organic frameworks (MOFs) gives rise to the development of advanced electrochemical sensors. However, integrating chirality by directly connecting metal ions and chiral ligands is unpredictable. Postmodification synthesis is a common method for synthesizing chiral MOFs, but it reduces the size of chiral channels and poses obstacles to the approach of chiral guest molecules. In this work, missing connection defects were introduced into the chiral MOFs through defect engineering strategies, which enhance the recognition of the target enantiomers. pH can tune enantioselectivity reversal in defective chiral MOFs. The chiral MOFs show enantioselectivity for d-Trp at pH = 5 and l-Trp at pH = 8. From the results of zeta potential, regardless of pH 5 or 8, the chiral MOF has a positive potential. The chiral MOFs are positively charged, while tryptophan is negatively charged when pH = 8. The difference in the positive and negative charge interactions between the two amino acids and chiral MOFs leads to chiral recognition. However, the difference in π-π interaction between chiral MOF and Trp enantiomers mainly drives chiral recognition under pH = 5. This study paves a pathway for the synthesis of defective chiral MOFs and highlights the pH-tuned enantioselectivity reversal.
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Affiliation(s)
- Xiaohui Niu
- College of Petrochemical Technology, Lanzhou University of Technology, Lanzhou 730050, PR China
| | - Mei Yuan
- College of Petrochemical Technology, Lanzhou University of Technology, Lanzhou 730050, PR China
| | - Rui Zhao
- College of Petrochemical Technology, Lanzhou University of Technology, Lanzhou 730050, PR China
| | - Yongqi Liu
- College of Petrochemical Technology, Lanzhou University of Technology, Lanzhou 730050, PR China
| | - Luhua Wang
- College of Petrochemical Technology, Lanzhou University of Technology, Lanzhou 730050, PR China
| | - Zengwei Pang
- College of Petrochemical Technology, Lanzhou University of Technology, Lanzhou 730050, PR China
| | - Shenteng Wan
- College of Petrochemical Technology, Lanzhou University of Technology, Lanzhou 730050, PR China
| | - Hongfang Zhao
- College of Petrochemical Technology, Lanzhou University of Technology, Lanzhou 730050, PR China
| | - Hongxia Li
- College of Petrochemical Technology, Lanzhou University of Technology, Lanzhou 730050, PR China
| | - Kunjie Wang
- College of Petrochemical Technology, Lanzhou University of Technology, Lanzhou 730050, PR China
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