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Zhang G, Lyu X, Qin Y, Li Y, Fan Z, Meng X, Cheng Y, Cao Z, Xu Y, Sun D, Gao Y, Gong Q, Lyu G. High discrimination ratio, broadband circularly polarized light photodetector using dielectric achiral nanostructures. LIGHT, SCIENCE & APPLICATIONS 2024; 13:275. [PMID: 39327415 PMCID: PMC11427471 DOI: 10.1038/s41377-024-01634-8] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 05/15/2024] [Revised: 08/29/2024] [Accepted: 09/08/2024] [Indexed: 09/28/2024]
Abstract
The on-chip measurement of polarization states plays an increasingly crucial role in modern sensing and imaging applications. While high-performance monolithic linearly polarized photodetectors have been extensively studied, integrated circularly polarized light (CPL) photodetectors are still hindered by inadequate discrimination capability. This study presents a broadband CPL photodetector utilizing achiral all-dielectric nanostructures, achieving an impressive discrimination ratio of ~107 at a wavelength of 405 nm. Our device shows outstanding CPL discrimination capability across the visible band without requiring intensity calibration. It functions based on the CPL-dependent near-field modes within achiral structures: under left or right CPL illumination, distinct near-field modes are excited, resulting in asymmetric irradiation of the two electrodes and generating a photovoltage with directions determined by the chirality of the incident light field. The proposed design strategy facilitates ultra-compact CPL detection across diverse materials, structures, and spectral ranges, presenting a novel avenue for achieving high-performance monolithic CPL detection.
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Affiliation(s)
- Guanyu Zhang
- State Key Laboratory for Mesoscopic Physics, Collaborative Innovation Center of Quantum Matter, Frontiers Science Center for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China
| | - Xiaying Lyu
- State Key Laboratory for Mesoscopic Physics, Collaborative Innovation Center of Quantum Matter, Frontiers Science Center for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China
| | - Yulu Qin
- State Key Laboratory for Mesoscopic Physics, Collaborative Innovation Center of Quantum Matter, Frontiers Science Center for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China
| | - Yaolong Li
- State Key Laboratory for Mesoscopic Physics, Collaborative Innovation Center of Quantum Matter, Frontiers Science Center for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China
| | - Zipu Fan
- International Center for Quantum Materials, School of Physics, Peking University, Beijing, China
| | - Xianghan Meng
- State Key Laboratory for Mesoscopic Physics, Collaborative Innovation Center of Quantum Matter, Frontiers Science Center for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China
| | - Yuqing Cheng
- School of Mathematics and Physics, University of Science and Technology Beijing, Beijing, China.
| | - Zini Cao
- State Key Laboratory for Mesoscopic Physics, Collaborative Innovation Center of Quantum Matter, Frontiers Science Center for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China
| | - Yixuan Xu
- State Key Laboratory for Mesoscopic Physics, Collaborative Innovation Center of Quantum Matter, Frontiers Science Center for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China
| | - Dong Sun
- International Center for Quantum Materials, School of Physics, Peking University, Beijing, China
| | - Yunan Gao
- State Key Laboratory for Mesoscopic Physics, Collaborative Innovation Center of Quantum Matter, Frontiers Science Center for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China
- Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan, Shanxi, China
- Peking University Yangtze Delta Institute of Optoelectronics, Nantong, Jiangsu, China
| | - Qihuang Gong
- State Key Laboratory for Mesoscopic Physics, Collaborative Innovation Center of Quantum Matter, Frontiers Science Center for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China
- Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan, Shanxi, China
- Peking University Yangtze Delta Institute of Optoelectronics, Nantong, Jiangsu, China
| | - Guowei Lyu
- State Key Laboratory for Mesoscopic Physics, Collaborative Innovation Center of Quantum Matter, Frontiers Science Center for Nano-Optoelectronics, School of Physics, Peking University, Beijing, China.
- Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan, Shanxi, China.
- Peking University Yangtze Delta Institute of Optoelectronics, Nantong, Jiangsu, China.
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Ahmed H, Ansari MA, Paterson L, Li J, Chen X. Metasurface for Engineering Superimposed Ince-Gaussian Beams. ADVANCED MATERIALS (DEERFIELD BEACH, FLA.) 2024; 36:e2312853. [PMID: 38353164 DOI: 10.1002/adma.202312853] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/28/2023] [Revised: 01/22/2024] [Indexed: 02/20/2024]
Abstract
Ince-Gaussian beams (IGBs) are the third complete family of exact and orthogonal solutions of the paraxial wave equation and have been applied in many fields ranging from particle trapping to quantum optics. IGBs play a very important role in optics as they represent the exact and continuous transition modes connecting Laguerre-Gaussian and Hermite-Gaussian beams. The method currently in use suffers from the high cost, complexity, and large volume of the optical system. The superposition of IGBs can generate complicated structured beams with multiple phase and polarization singularities. A metasurface approach is proposed to realizing various superpositions of IGBs without relying on a complicated optical setup. By superimposing IGBs with even and odd modes, multiple phase, and polarization singularities are observed in the resultant beams. The phase and polarization singularities are modulated by setting the initial phase in the design and controlling the incident linear polarization. The compactness of the developed metasurface devices and the unique properties of the generated beams have the potential to impact many practical applications such as particle manipulation, orbital angular momentum spectrum manipulation, and optical communications.
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Affiliation(s)
- Hammad Ahmed
- Institute of Photonics and Quantum Sciences, School of Engineering and Physical Sciences, Heriot-Watt University, Edinburgh, EH14 4AS, UK
| | - Muhammad Afnan Ansari
- Institute of Photonics and Quantum Sciences, School of Engineering and Physical Sciences, Heriot-Watt University, Edinburgh, EH14 4AS, UK
| | - Lynn Paterson
- Institute of Biological Chemistry, Biophysics and Bioengineering, School of Engineering and Physical Sciences, Heriot-Watt University, Edinburgh, EH14 4AS, UK
| | - Jia Li
- Shenzhen Key Laboratory of Ultraintense Laser and Advanced Material Technology, Center for Advanced Material Diagnostic Technology, and College of Engineering Physics, Shenzhen Technology University, Shenzhen, 518118, China
| | - Xianzhong Chen
- Institute of Photonics and Quantum Sciences, School of Engineering and Physical Sciences, Heriot-Watt University, Edinburgh, EH14 4AS, UK
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Wang S, Hu T, Wang S, Wei Y, Mei Z, Yan B, Zhou W, Yang Z, Zheng J, Peng Y, Zhao M. Full Stokes polarimetry based on an inverse-designed multi-foci metalens. OPTICS LETTERS 2024; 49:1595-1598. [PMID: 38489459 DOI: 10.1364/ol.516135] [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: 02/23/2024] [Indexed: 03/17/2024]
Abstract
In the realm of metasurface-based polarimetry, well-known for its remarkable compactness and integration capabilities, previous attempts have been hindered by limitations such as the restricted choices of target polarization states and the inefficient focusing of light. To address these problems, this study introduces and harnesses a novel, to our knowledge, forward-solving model, grounded in the equivalence principle and dyadic Green's function, to inversely optimize the vectorial focusing patterns of metalenses. Leveraging this methodology, we develop and experimentally validate a single multi-foci metalens-based polarimeter, capable of simultaneously separating and concentrating four distinct elliptical polarization states at a wavelength of 10.6 µm. Rigorous experimental evaluations, involving the assessment of 18 scalar polarized beams, reveal an average error of 5.92% and a high contrast ratio of 0.92, which demonstrates the efficacy of the polarimeter. The results underscore the potential of our system in diverse sectors, including military defense, healthcare, and autonomous vehicle technology.
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Tian S, Yuan W, Guo J, Chen Q, Chen Y. Dual layer chessboard metasurface sandwiched by a spin-on-carbon for spectral modulation. OPTICS EXPRESS 2024; 32:5022-5030. [PMID: 38439239 DOI: 10.1364/oe.514762] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/29/2023] [Accepted: 01/19/2024] [Indexed: 03/06/2024]
Abstract
Metasurfaces, composed by metals and dielectrics in periodical order with subwavelength pitches, are of great importance for their unique ability to abruptly manipulate optical fields. So far, all the reported metasurfaces are constructed by thermally deposited metals and dielectric films, based on semiconductor processes which are expensive and time-consuming. Inspired by the outstanding dry etch property of spin-on-carbon (SOC) as the interlayer material in CMOS technology, this paper proposes to utilize the SOC as the dielectric layer in a chessboard metasurface with dual layer of gold to form an array of local surface plasmonic resonators (localized surface plasmon resonance). Finite difference and time domain (FDTD) method is used to investigate the spectral characteristics in reflectance of the metasurface in both visible and short wavelengths of infrared light. Electron beam lithography is applied to generate the nanoscale chessboard pattern on ZEP520A, followed by a conventional oxygen-based plasma etch to form high aspect ratio nanopillar arrays in SOC with the feature width under 50 nm, and ended by a thermal deposition of gold to form self-aligned dual layer local surface plasmonic resonators (LSPRs). The measured reflectance spectra agree with the simulated. A wealth of optical properties, such as coupling induced modulations of spectra by LSPRs, are revealed and analyzed. These special modes result in tunable structural colors and wavelength-selective antireflection ability. To the best of our knowledge, this is the first time that SOC is applied in the construction of metasurfaces, which has great potential for next generation nanophotonic devices.
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Zuo J, Bai J, Choi S, Basiri A, Chen X, Wang C, Yao Y. Chip-integrated metasurface full-Stokes polarimetric imaging sensor. LIGHT, SCIENCE & APPLICATIONS 2023; 12:218. [PMID: 37673857 PMCID: PMC10482842 DOI: 10.1038/s41377-023-01260-w] [Citation(s) in RCA: 14] [Impact Index Per Article: 7.0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/29/2023] [Revised: 07/27/2023] [Accepted: 08/09/2023] [Indexed: 09/08/2023]
Abstract
Polarimetric imaging has a wide range of applications for uncovering features invisible to human eyes and conventional imaging sensors. Chip-integrated, fast, cost-effective, and accurate full-Stokes polarimetric imaging sensors are highly desirable in many applications, which, however, remain elusive due to fundamental material limitations. Here we present a chip-integrated Metasurface-based Full-Stokes Polarimetric Imaging sensor (MetaPolarIm) realized by integrating an ultrathin (~600 nm) metasurface polarization filter array (MPFA) onto a visible imaging sensor with CMOS compatible fabrication processes. The MPFA is featured with broadband dielectric-metal hybrid chiral metasurfaces and double-layer nanograting polarizers. This chip-integrated polarimetric imaging sensor enables single-shot full-Stokes imaging (speed limited by the CMOS imager) with the most compact form factor, records high measurement accuracy, dual-color operation (green and red) and a field of view up to 40 degrees. MetaPolarIm holds great promise to enable transformative applications in autonomous vision, industry inspection, space exploration, medical imaging and diagnosis.
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Grants
- 2048230 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- 1809997 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- ECCS-1542160 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- 2048230 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- 1809997 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- ECCS-1542160 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- 2048230 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- 1809997 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- ECCS-1542160 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- 2048230 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- 1809997 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- ECCS-1542160 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- 2048230 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- 1809997 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- ECCS-1542160 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- 2048230 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- 1809997 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- ECCS-1542160 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- 2048230 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- 1809997 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- ECCS-1542160 NSF | ENG/OAD | Division of Electrical, Communications and Cyber Systems (ECCS)
- DE-EE0008999 DOE | Advanced Research Projects Agency - Energy (Advanced Research Projects Agency - Energy - U.S. Department of Energy)
- DE-EE0008999 DOE | Advanced Research Projects Agency - Energy (Advanced Research Projects Agency - Energy - U.S. Department of Energy)
- DE-EE0008999 DOE | Advanced Research Projects Agency - Energy (Advanced Research Projects Agency - Energy - U.S. Department of Energy)
- DE-EE0008999 DOE | Advanced Research Projects Agency - Energy (Advanced Research Projects Agency - Energy - U.S. Department of Energy)
- DE-EE0008999 DOE | Advanced Research Projects Agency - Energy (Advanced Research Projects Agency - Energy - U.S. Department of Energy)
- DE-EE0008999 DOE | Advanced Research Projects Agency - Energy (Advanced Research Projects Agency - Energy - U.S. Department of Energy)
- DE-EE0008999 DOE | Advanced Research Projects Agency - Energy (Advanced Research Projects Agency - Energy - U.S. Department of Energy)
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Affiliation(s)
- Jiawei Zuo
- School of Electrical, Computer and Energy Engineering, Arizona State University, 85281, Tempe, AZ, USA
- Center for Photonic Innovation, Arizona State University, 85281, Tempe, AZ, USA
| | - Jing Bai
- School of Electrical, Computer and Energy Engineering, Arizona State University, 85281, Tempe, AZ, USA
- Center for Photonic Innovation, Arizona State University, 85281, Tempe, AZ, USA
| | - Shinhyuk Choi
- School of Electrical, Computer and Energy Engineering, Arizona State University, 85281, Tempe, AZ, USA
- Center for Photonic Innovation, Arizona State University, 85281, Tempe, AZ, USA
| | - Ali Basiri
- School of Electrical, Computer and Energy Engineering, Arizona State University, 85281, Tempe, AZ, USA
- Center for Photonic Innovation, Arizona State University, 85281, Tempe, AZ, USA
| | - Xiahui Chen
- School of Electrical, Computer and Energy Engineering, Arizona State University, 85281, Tempe, AZ, USA
- Center for Photonic Innovation, Arizona State University, 85281, Tempe, AZ, USA
| | - Chao Wang
- School of Electrical, Computer and Energy Engineering, Arizona State University, 85281, Tempe, AZ, USA
- Center for Photonic Innovation, Arizona State University, 85281, Tempe, AZ, USA
- Biodesign Center for Molecular Design and Biomimetics, Arizona State University, 85281, Tempe, AZ, USA
| | - Yu Yao
- School of Electrical, Computer and Energy Engineering, Arizona State University, 85281, Tempe, AZ, USA.
- Center for Photonic Innovation, Arizona State University, 85281, Tempe, AZ, USA.
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Wang X, Zhu K, Zhu K, Li B, Shen D, Zheng ZG. A simple polarimetric measurement based on a computational algorithm. OPTICS LETTERS 2023; 48:4085-4088. [PMID: 37527124 DOI: 10.1364/ol.494727] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 05/05/2023] [Accepted: 07/02/2023] [Indexed: 08/03/2023]
Abstract
A simple and compact polarimeter comprising two electrically controlled liquid-crystal variable retarders (LCVRs) and a linear polarizer is demonstrated, which is enabled by analyzing the intensity variation of the modulated output light based on a computational algorithm. A proof-of-concept prototype is presented, which is mounted onto a power meter or a CMOS camera for the intensity data collection. The polarimetric measurement for the spatial variant polarization states of light is also verified, indicating the possibility of achieving a resolution-lossless polarimeter. Thus, our proposed method shows a cost-effective way to realize a compact polarimeter in polarization optics.
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Qu J, Wang Z, Cehng Z, Wang Y, Yu C. Full-Stokes parameters detection enabled by a non-interleaved fiber-compatible metasurface. OPTICS EXPRESS 2023; 31:20836-20849. [PMID: 37381198 DOI: 10.1364/oe.491836] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/04/2023] [Accepted: 05/20/2023] [Indexed: 06/30/2023]
Abstract
Polarization of the optical field determines the way of light-matter interaction, which lays the foundation for various applications such as chiral spectroscopy, biomedical imaging, and machine vision. Currently, with the rise of the metasurface, miniaturized polarization detectors have attracted extensive interest. However, due to the limitation of the working area, it is still a challenge to integrate polarization detectors on the fiber end face. Here, we propose a design of compact non-interleaved metasurface that can be integrated on the tip of a large-mode-area photonic crystal fiber (LMA-PCF) to realize full-Stokes parameters detection. Through concurrent control over the dynamic phase and Pancharatnam-Berry (PB) phase, different helical phases are assigned to the two orthogonal circular polarization bases, of which the amplitude contrast and relative phase difference can be represented by two non-overlapped foci and an interference ring pattern, respectively. Therefore, the determination of arbitrary polarization states through the proposed ultracompact fiber-compatible metasurface can be achieved. Moreover, we calculated full-Stokes parameters according to simulation results and obtained that the average detection deviation is relatively low at 2.84% for 20 elucidated samples. The novel metasurface exhibits excellent polarization detection performance and overcomes the limitation of the small integrated area, which provides insights into the further practical explorations of ultracompact polarization detection devices.
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