Yuting Xiao 1,2,4†Lianwei Chen 1,2,3,4†Mingbo Pu 1,2,3,4,*Mingfeng Xu 1,2,3,4[ ... ]Xiangang Luo 1,2,4,**
Author Affiliations
Abstract
1 National Key Laboratory of Optical Field Manipulation Science and Technology, Chinese Academy of Sciences, Chengdu 610209, China
2 State Key Laboratory of Optical Technologies on Nano-Fabrication and Micro-Engineering, Institute of Optics and Electronics, Chinese Academy of Sciences, Chengdu 610209, China
3 Research Center on Vector Optical Fields, Institute of Optics and Electronics, Chinese Academy of Sciences, Chengdu 610209, China
4 School of Optoelectronics, University of Chinese Academy of Sciences, Beijing 100049, China
Super-resolution (SR) microscopy has dramatically enhanced our understanding of biological processes. However, scattering media in thick specimens severely limits the spatial resolution, often rendering the images unclear or indistinguishable. Additionally, live-cell imaging faces challenges in achieving high temporal resolution for fast-moving subcellular structures. Here, we present the principles of a synthetic wave microscopy (SWM) to extract three-dimensional information from thick unlabeled specimens, where photobleaching and phototoxicity are avoided. SWM exploits multiple-wave interferometry to reveal the specimen’s phase information in the area of interest, which is not affected by the scattering media in the optical path. SWM achieves ~0.42 λ/NA resolution at an imaging speed of up to 106 pixels/s. SWM proves better temporal resolution and sensitivity than the most conventional microscopes currently available while maintaining exceptional SR and anti-scattering capabilities. Penetrating through the scattering media is challenging for conventional imaging techniques. Remarkably, SWM retains its efficacy even in conditions of low signal-to-noise ratios. It facilitates the visualization of dynamic subcellular structures in live cells, encompassing tubular endoplasmic reticulum (ER), lipid droplets, mitochondria, and lysosomes.
super-resolution anti-scattering unlabeled high temporal resolution 
Opto-Electronic Science
2023, 2(11): 230037
Yingli Ha 1,2,3†Yu Luo 1,2,3†Mingbo Pu 1,2,3,4,*Fei Zhang 1,2,3[ ... ]Xiangang Luo 1,2,3,4,**
Author Affiliations
Abstract
1 National Key Laboratory of Optical Field Manipulation Science and Technology, Chinese Academy of Sciences, Chengdu 610209, China
2 State Key Laboratory of Optical Technologies on Nano-Fabrication and Micro-Engineering, Institute of Optics and Electronics, Chinese Academy of Sciences, Chengdu 610209, China
3 Research Center on Vector Optical Fields, Institute of Optics and Electronics, Chinese Academy of Sciences, Chengdu 610209, China
4 School of Optoelectronics, University of Chinese Academy of Sciences, Beijing 100049, China
5 Tianfu Xinglong Lake Laboratory, Chengdu 610299, China
Metalenses have gained significant attention and have been widely utilized in optical systems for focusing and imaging, owing to their lightweight, high-integration, and exceptional-flexibility capabilities. Traditional design methods neglect the coupling effect between adjacent meta-atoms, thus harming the practical performance of meta-devices. The existing physical/data-driven optimization algorithms can solve the above problems, but bring significant time costs or require a large number of data-sets. Here, we propose a physics-data-driven method employing an “intelligent optimizer” that enables us to adaptively modify the sizes of the meta-atom according to the sizes of its surrounding ones. The implementation of such a scheme effectively mitigates the undesired impact of local lattice coupling, and the proposed network model works well on thousands of data-sets with a validation loss of 3×10?3. Based on the “intelligent optimizer”, a 1-cm-diameter metalens is designed within 3 hours, and the experimental results show that the 1-mm-diameter metalens has a relative focusing efficiency of 93.4% (compared to the ideal focusing efficiency) and a Strehl ratio of 0.94. Compared to previous inverse design method, our method significantly boosts designing efficiency with five orders of magnitude reduction in time. More generally, it may set a new paradigm for devising large-aperture meta-devices.
intelligence method physics-data-driven method inverse design large-aperture metalenses 
Opto-Electronic Advances
2023, 6(11): 230133
Yiqun Zhang 1,2†Mingfeng Xu 2,3†Mingbo Pu 2,3,4Mengjie Zhou 5[ ... ]Xiangang Luo 2,4,*
Author Affiliations
Abstract
1 School of Information and Communication Engineering, University of Electronic Science and Technology of China, Chengdu 611731, China
2 State Key Laboratory of Optical Technologies on Nano-Fabrication and Micro-Engineering, Institute of Optics and Electronics, Chinese Academy of Sciences, Chengdu 610209, China
3 Research Center on Vector Optical Fields, Institute of Optics and Electronics, Chinese Academy of Sciences, Chengdu 610209, China
4 School of Optoelectronics, University of Chinese Academy of Sciences, Beijing 100049, China
5 Tianfu Xinglong Lake Laboratory, Chengdu 610299, China
6 e-mail: uestc_nj@uestc.edu.cn
Optical chaotic signals emitted from an external-cavity feedback or injected laser diode enable small-signal information concealment in a noise-like carrier for secure optical communications. Due to the chaotic bandwidth limitation resulting from intrinsic relaxation oscillation frequency of lasers, multiplexing of optical chaotic signal, such as wavelength division multiplexing in fiber, is a typical candidate for high-capacity secure applications. However, to our best knowledge, the utilization of the spatial dimension of optical chaos for free-space secure communication has not yet been reported. Here, we experimentally demonstrate a free-space all-optical chaotic communication system that simultaneously enhances transmission capacity and security by orbital angular momentum (OAM) multiplexing. Optical chaotic signals with two different OAM modes totally carrying 20 Gbps on–off keying signals are secretly transmitted over a 2 m free-space link, where the channel crosstalk of OAM modes is less than -20 dB, with the mode spacing no less than 3. The receiver can extract valid information only when capturing approximately 92.5% of the OAM beam and correctly demodulating the corresponding mode. Bit error rate below the 7% hard-decision forward error correction threshold of 3.8×10-3 can be achieved for the intended recipient. Moreover, a simulated weak turbulence is introduced to comprehensively analyze the influence on the system performance, including channel crosstalk, chaotic synchronization, and transmission performance. Our work may inspire structured light application in optical chaos and pave a new way for developing future high-capacity free-space chaotic secure communication systems.
Photonics Research
2023, 11(12): 2185
Mingbo Pu 1,2,3,4Xiangang Luo 1,2,3,4,*
Author Affiliations
Abstract
1 State Key Laboratory of Optical Technologies on Nano-Fabrication and Micro-Engineering, Institute of Optics and Electronics, Chinese Academy of Sciences, Chengdu 610209, China
2 Key Laboratory of Optical Field Manipulation Science and Technology, Chinese Academy of Sciences, Chengdu 610209, China
3 Research Center on Vector Optical Fields, Institute of Optics and Electronics, Chinese Academy of Sciences, Chengdu 610209, China
4 School of Optoelectronics, University of Chinese Academy of Sciences, Beijing 100049, China
Dielectric metasurfaces are crucial for enhancing optical nonlinear generation, particularly membrane metasurfaces with multipolar resonances and compact size. Investigating silicon dimer-hole membrane metasurfaces, Rahmani, and Xu show how bound states in the continuum (BICs) can be formed and transformed into quasi-BICs by adjusting hole gaps. This innovation enables efficient conversion of infrared images to visible range, promising applications in nonlinear photonics and near-infrared imaging technologies.
Opto-Electronic Advances
2023, 6(8): 230153
邓泉 1,2赵泽宇 1,2林鹤 1,3刘玲 1,2[ ... ]罗先刚 1,2,*
作者单位
摘要
1 中国科学院光电技术研究所微细加工光学技术国家重点实验室,四川 成都 610209
2 中国科学院大学光电学院,北京 100049
3 电子科技大学自动化工程学院,四川 成都 610054
缺陷检测是基于金属膜层激发表面等离子体进行超衍射加工前的重要工艺流程,但目前先进空白晶圆缺陷检测设备光源多位于深紫外波段,恰好在KrF等深紫外光刻胶的感光范围内,检测带有该光刻胶的晶圆表面时易导致光刻胶感光而改性失效。针对此问题,笔者提出并设计了一种基于可见光波段的激光偏振暗场检测装置。该装置利用晶圆表面顶层银膜的偏振转换特性,通过调控入射光的偏振态与入射角,使微粗糙银膜表面的弱散射光偏振态与膜层表面颗粒的散射光偏振态产生差异,然后利用偏振器件对来自银膜表面的散射光进行部分滤除,有效提高了颗粒信号的信噪比。实验结果表明:所设计的装置在不影响光刻胶的同时还可以减少金属膜层表面散射所带来的缺陷误检。在对百纳米级颗粒进行检测时,由于使用了激光照明及高灵敏度的sCMOS作为探测器件,本装置单次曝光时间仅为150 μs,是奥林巴斯公司基于白光的DSX1000暗场显微镜的4‰左右。通过抑制噪声,笔者采用该装置实测了均方根(RMS)粗糙度为3.4 nm的银膜表面上直径为61 nm的聚苯乙烯乳胶颗粒,结果显示,该装置在探测极限和探测效率上较DSX1000均有较大提升。
测量 光学检测 散射测量 表面粗糙度 偏振调控 纳米颗粒 信噪比 
中国激光
2023, 50(22): 2204003
张作蛟 1,2方瑶 1王青松 1李雄 1,2[ ... ]罗先刚 1,2,*
作者单位
摘要
1 中国科学院光电技术研究所微细加工光学技术国家重点实验室,四川 成都 610209
2 中国科学院大学,北京 100049
3 中国科学院光电技术研究所矢量光场研究中心,四川 成都 610209
高阶贝塞尔光束能够携带轨道角动量,且具有无衍射特性,在粒子操控、激光微纳加工及非线性光学等领域具有重要应用价值。目前产生高阶贝塞尔光束的方式无法同时满足集成化和高功率场景的应用需求。基于飞秒激光诱导的双折射纳米光栅结构,提出一种高损伤阈值的集成化光场调控器件制备方法。通过调控纳米光栅的光轴方向和相位延迟量,在石英玻璃内部写入光轴取向空间变化的多层纳米光栅结构,制备的器件可以实现不同光场调控功能的叠加和不同工作波长的设计。基于所提方法制备了中心波长为532 nm、拓扑荷值为4的高阶贝塞尔光束产生器件。器件产生的高阶贝塞尔光束携带的轨道角动量与设计值相符,在4 m距离内光斑大小保持基本不变。器件的零几率激光损伤阈值为28.5 J/cm2(6 ns),在高功率激光光束整形等领域具有极大的应用潜力。
激光光场调控 高阶贝塞尔光束 集成化光学元件 飞秒激光 纳米光栅 激光损伤阈值 
光学学报
2023, 43(13): 1326003
黄远建 1,2李晓银 1,2叶文怡 1,2郭迎辉 1,2[ ... ]罗先刚 1,2,*
作者单位
摘要
1 中国科学院光电技术研究所微细加工光学技术国家重点实验室,四川 成都 610209
2 中国科学院大学电子电气与通信工程学院,北京 101408
3 天府兴隆湖实验室,四川 成都 610299
激光雷达技术因具有高精度、高分辨率和工作距离远等优点被广泛应用于三维成像。然而,受光学系统衍射极限的限制,激光雷达的空间分辨率随着目标距离的增大而显著降低。为解决上述问题,结合共聚焦照明技术和亚像素扫描技术,提出一种聚焦照明亚像素扫描光子计数激光雷达,并在实验室内进行了10 m成像实验。结果表明,相较于准直照明光束,采用共聚焦照明光束可将系统空间分辨率由5.0 mm提高到0.9 mm,不仅实现了超光学系统衍射极限成像,还有效降低了多重回波的影响,增强了回波强度。
光学设计 激光雷达 亚像素扫描 共聚焦照明 高分辨率 
光学学报
2023, 43(8): 0822014
作者单位
摘要
光学学报
2023, 43(8): 0822000
Yunsong Lei 1,2†Qi Zhang 1,2†Yinghui Guo 1,2Mingbo Pu 1,2[ ... ]Xiangang Luo 1,2,*
Author Affiliations
Abstract
1 State Key Laboratory of Optical Technologies on Nano-Fabrication and Micro-Engineering, Institute of Optics and Electronics, Chinese Academy of Sciences, Chengdu 610209, China
2 School of Optoelectronics, University of Chinese Academy of Sciences, Beijing 100049, China
3 Tianfu Xinglong Lake Laboratory, Chengdu 610299, China
Multi-dimensional optical imaging systems that simultaneously gather intensity, depth, polarimetric, and spectral information have numerous applications in medical sciences, robotics, and surveillance. Nevertheless, most current approaches require mechanical moving parts or multiple modulation processes and thus suffer from long acquisition time, high system complexity, or low sampling resolution. Here, a methodology to build snapshot multi-dimensional lensless imaging is proposed by combining planar-optics and computational technology, benefiting from sufficient flexibilities in optical engineering and robust information reconstructions. Specifically, a liquid crystal diffuser based on geometric phase modulation is designed to simultaneously encode the spatial, spectral, and polarization information of an object into a snapshot detected speckle pattern. At the same time, a post-processing algorithm acts as a special decoder to recover the hidden information in the speckle with the independent and unique point spread function related to the position, wavelength, and chirality. With the merits of snapshot acquisition, multi-dimensional perception ability, simple optical configuration, and compact device size, our approach can find broad potential applications in object recognition and classification.
Photonics Research
2023, 11(3): B111
Author Affiliations
Abstract
Imaging polarimetry is one of the most widely used analytical technologies for object detection and analysis. To date, most metasurface-based polarimetry techniques are severely limited by narrow operating bandwidths and inevitable crosstalk, leading to detrimental effects on imaging quality and measurement accuracy. Here, we propose a crosstalk-free broadband achromatic full Stokes imaging polarimeter consisting of polarization-sensitive dielectric metalenses, implemented by the principle of polarization-dependent phase optimization. Compared with the single-polarization optimization method, the average crosstalk has been reduced over three times under incident light with arbitrary polarization ranging from 9 μm to 12 μm, which guarantees the measurement of the polarization state more precisely. The experimental results indicate that the designed polarization-sensitive metalenses can effectively eliminate the chromatic aberration with polarization selectivity and negligible crosstalk. The measured average relative errors are 7.08%, 8.62%, 7.15%, and 7.59% at 9.3, 9.6, 10.3, and 10.6 μm, respectively. Simultaneously, the broadband full polarization imaging capability of the device is also verified. This work is expected to have potential applications in wavefront detection, remote sensing, light-field imaging, and so forth.Imaging polarimetry is one of the most widely used analytical technologies for object detection and analysis. To date, most metasurface-based polarimetry techniques are severely limited by narrow operating bandwidths and inevitable crosstalk, leading to detrimental effects on imaging quality and measurement accuracy. Here, we propose a crosstalk-free broadband achromatic full Stokes imaging polarimeter consisting of polarization-sensitive dielectric metalenses, implemented by the principle of polarization-dependent phase optimization. Compared with the single-polarization optimization method, the average crosstalk has been reduced over three times under incident light with arbitrary polarization ranging from 9 μm to 12 μm, which guarantees the measurement of the polarization state more precisely. The experimental results indicate that the designed polarization-sensitive metalenses can effectively eliminate the chromatic aberration with polarization selectivity and negligible crosstalk. The measured average relative errors are 7.08%, 8.62%, 7.15%, and 7.59% at 9.3, 9.6, 10.3, and 10.6 μm, respectively. Simultaneously, the broadband full polarization imaging capability of the device is also verified. This work is expected to have potential applications in wavefront detection, remote sensing, light-field imaging, and so forth.
metasurface broadband achromatic crosstalk-free full polarization imaging polarimetry 
Opto-Electronic Advances
2022, 5(11): 220058

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