Jianbin Zhang 1†Hubiao Fang 1Pan Wang 1,2Wei Fang 1,2[ ... ]Limin Tong 1,2,3,*
Author Affiliations
Abstract
1 Interdisciplinary Center for Quantum Information, New Cornerstone Science Laboratory, State Key Laboratory of Extreme Photonics and Instrumentation, College of Optical Science and Engineering, Zhejiang University, Hangzhou, China
2 Jiaxing Key Laboratory of Photonic Sensing & Intelligent Imaging, Intelligent Optics & Photonics Research Center, Jiaxing Research Institute Zhejiang University, Jiaxing, China
3 Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan, China
An optical micro/nanofiber (MNF) is a quasi-one-dimensional free-standing optical waveguide with a diameter close to or less than the vacuum wavelength of light. Combining the tiny geometry with high-refractive-index contrast between the core and the surrounding, the MNF exhibits favorable optical properties such as tight optical confinement, strong evanescent field, and large-diameter-dependent waveguide dispersion. Meanwhile, as a quasi-one-dimensional structure with extraordinarily high geometric and structural uniformity, the MNF also has low optical loss and high mechanical strength, making it favorable for manipulating light on the micro/nanoscale with high flexibility. Over the past two decades, optical MNFs, typically being operated in single mode, have been emerging as a miniaturized fiber-optic platform for both scientific research and technological applications. In this paper, we aim to provide a comprehensive overview of the representative advances in optical MNFs in recent years. Starting from the basic structures and fabrication techniques of the optical MNFs, we highlight linear and nonlinear optical and mechanical properties of the MNFs. Then, we introduce typical applications of optical MNFs from near-field optics, passive optical components, optical sensors, and optomechanics to fiber lasers and atom optics. Finally, we give a brief summary of the current status of MNF optics and technology, and provide an outlook into future challenges and opportunities.
micro/nanofibers fabrication optical properties mechanical properties optical applications 
Photonics Insights
2024, 3(1): R02
Yuxin Yang 1†Jiaxin Gao 1†Hao Wu 1Zhanke Zhou 1[ ... ]Limin Tong 1,2,3,5,*
Author Affiliations
Abstract
1 Interdisciplinary Center for Quantum Information, New Cornerstone Science Laboratory, State Key Laboratory of Extreme Photonics and Instrumentation, College of Optical Science and Engineering, Zhejiang University, Hangzhou 310027, China
2 Jiaxing Key Laboratory of Photonic Sensing & Intelligent Imaging, Intelligent Optics & Photonics Research Center, Jiaxing Research Institute Zhejiang University, Jiaxing 314000, China
3 Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan 030006, China
4 e-mail: guoxin@zju.edu.cn
5 e-mail: phytong@zju.edu.cn
An optical field with sub-nm confinement is essential for exploring atomic- or molecular-level light-matter interaction. While such fields demonstrated so far have typically point-like cross-sections, an optical field having a higher-dimensional cross-section may offer higher flexibility and/or efficiency in applications. Here, we propose generating a nanoscale blade-like optical field in a coupled nanofiber pair (CNP) with a 1-nm-width central slit. Based on a strong mode coupling-enabled slit waveguide mode, a sub-nm-thickness blade-like optical field can be generated with a cross-section down to 0.28 nm×38 nm at 1550 nm wavelength (i.e., a thickness of λ0/5000) and a peak-to-background intensity ratio (PBR) higher than 20 dB. The slit waveguide mode of the CNP can be launched from one of the two nanofibers that are connected to a standard optical fiber via an adiabatical fiber taper, in which a fundamental waveguide mode of the fiber can be converted into a high-purity slit mode with high efficiency (>98%) within a CNP length of less than 10 μm at 1550 nm wavelength. The wavelength-dependent behaviors and group velocity dispersion in mode converting processes are also investigated, showing that such a CNP-based design is also suitable for broadband and ultrafast pulsed operation. Our results may open up new opportunities for studying light-matter interaction down to the sub-nm scale, as well as for exploring ultra-high-resolution optical technology ranging from super-resolution nanoscopy to chemical bond manipulation.
Photonics Research
2024, 12(1): 154
作者单位
摘要
中国科学院长春光学精密机械与物理研究所,吉林 长春130033
针对实时高效处理经纬仪交会数据的问题,提出了一种基于改进分布式处理平台的实时测角数据对齐及异步计算方法。分析了交会算法的耗时原理。根据交会数据实时性高、对时间复杂度过高的算法应用困难的特点,利用分布式平台对实时测角数据进行异步处理,并改进了传统同步交会数据处理流程。试验结果表明,改进分布式平台处理数据效率高,性能稳定,能够满足高时间复杂度算法的嵌入和实时处理需求。
分布式处理 交会 实时处理 异步计算 distributed processing rendezvous real-time processing asynchronous computing 
红外
2023, 44(11): 0036
作者单位
摘要
湖南工业大学计算机学院,湖南 株洲 412007
基于光纤布拉格光栅对(DFBGs)的双波长线形腔光纤激光器利用偏振烧孔效应实现双波长激光稳定输出的研究颇多,但有关3 dB光纤环形镜(FLM)与光纤布拉格光栅(FBG)构成腔镜或仅FBG构成腔镜,以及DFBGs的选择对其激光输出性能[光信噪比(OSNR)、斜率效率及稳定性等]的影响的研究很少。本文实验首先在双波长线形腔掺铒光纤激光器中比较了3 dB FLM与FBG构成腔镜和仅FBG构成腔镜的双波长激光的输出性能,结果表明,仅FBG构成腔镜的输出性能优于3 dB FLM与FBG构成腔镜的输出。其次在仅FBG构成腔镜的线形腔中对低反射率FBG(输出镜)反射率相同与不同时的输出性能进行了对比,研究表明,低反射率FBG的反射率相同时双波长激光输出具有较高的OSNR、斜率效率和稳定性。接着改变构成腔镜的两对FBG的中心波长间隔分别为4、8、12 nm,研究表明,中心波长间隔越大输出越稳定,OSNR越高,但激光器的斜率效率有所降低。最后在室温环境下实现了两个激光波长分别为1550 nm和1562 nm、OSNR分别为50.24 dB和51.19 dB左右、中心波长变化分别小于0.030 nm和0.035 nm、输出功率波动分别小于0.061 mW和0.059 mW、3 dB带宽分别为~0.146 nm和~0.144 nm的稳定输出,该结果为线形腔双波长的更优输出。
光纤布拉格光栅对 偏振烧孔 3 dB光纤环形镜 双波长线形腔掺铒光纤激光器 中心波长间隔 
光学学报
2023, 43(23): 2306005
作者单位
摘要
中国电子科技集团第二十七研究所, 河南 郑州 450047
从光学工程应用的角度对全国云量情况进行了研究,重点分析了全国陆地主要地区云量总体平均情况、冷暖半年、昼夜变化等三个方面云量历史数据,研究结果表明:全国陆地主要地区总云量和低云量分布区域基本呈北少南多的情况;冷暖半年云量分布有较明显的差别,暖半年云量高于冷半年的站点区域占全国较大面积;昼夜云量分布区别主要体现在西部地区白天低云低值区会有中高云存在。在云量总体平均情况、冷暖半年、昼夜变化的分析基础上进而讨论了全国云量区域的分级情况,结果表明适合光学工程应用的1级区主要分在北方。结果有助于了解全国适于开展光学工程应用的区域,并可为进一步研究云量对光学工程应用产生的定量影响提供参考。
光学工程 云量级别 总云量 低云量 冷暖半年 昼夜变化 optical engineering cloud cover levels total cloud cover low cloud cover cold and warm of half year diurnal variation 
大气与环境光学学报
2023, 18(5): 445
石峰 1,2,*程宏昌 1,2闫磊 1,2郭欣 1,2[ ... ]丁习文 1,2
作者单位
摘要
1 昆明物理研究所,云南昆明 650223
2 微光夜视技术重点实验室,陕西西安 710065
随着我国海洋、江河和地下水资源勘探、开发和利用的日益深入,以及领海主权防卫的**需求日趋迫切,在水下获取远距离条件下高质量的目标图像已成为水下环境勘测、目标探测与敌我对抗等许多领域迫切需要解决的问题。目前,水下成像探测技术主要有声探测和光电探测两种途径。本文研究了目前主要水下高分辨力光电探测成像技术现状,分析了不同技术途径的优缺点,对比了各种水下探测 /成像系统中采用的光电探测器的情况,结合自身技术背景,提出了应加快发展高灵敏度、低噪声、高增益、快响应、宽动态范围、良好线性度的 GaAsP光阴极双微通道板像增强器,从而简化光电系统中因探测器性能不佳带来的灵敏度低、噪声大、增益低、处理时间长等不足,加速各种新技术向产品、实用化设备的转化。本文成果对水下光电成像技术发展将有一定支撑作用。
水下探测 光电成像 探测器 underwater detection, photoelectric imaging, detec 
红外技术
2023, 45(10): 1066
郭欣 1,2石峰 2,*贾甜甜 2张若愚 2[ ... ]张益军 3
作者单位
摘要
1 北京理工大学 光电学院,北京 102401
2 微光夜视技术重点实验室,西安 710065
3 南京理工大学 电子工程与光电技术学院,南京 210094
为研究透射式GaAs光电阴极在不同波长入射光环境下的图像分辨能力,提出了一种基于散射传递函数的AlGaAs窗口层界面散射理论模型。制作了透射式GaAs光电阴极,利用不同波长入射光散射传递函数和点扩散函数变化,基于有参峰信噪比拟合对AlGaAs窗口层界面散射引起的入射光学图像退化程度进行了定量分析。结果表明,在相同的粗糙度下随着入射光波长的增加,入射光学图像的能量损失越小,成像质量越高,而三代微光像增强器不同波长入射光测试条件下极限分辨力变化趋势与仿真计算结果一致,可为后续提高透射式GaAs光电阴极分辨力提供了技术支撑。
光电阴极 GaAs 散射传递函数 波长 粗糙度 分辨力 Photocathode GaAs Scattering transfer function Wavelength Roughness Resolution 
光子学报
2023, 52(8): 0812001
Author Affiliations
Abstract
1 Zhejiang University, College of Optical Science and Engineering, New Cornerstone Science Laboratory, Interdisciplinary Center for Quantum Information, Hangzhou, China
2 Jiaxing Institute of Zhejiang University, Intelligent Optics and Photonics Research Center, Jiaxing, China
3 Shanxi University, Collaborative Innovation Center of Extreme Optics, Taiyuan, China
We propose to generate a sub-nanometer-confined optical field in a nanoslit waveguiding mode in a coupled nanowire pair (CNP). We show that, when a conventional waveguide mode with a proper polarization is evanescently coupled into a properly designed CNP with a central nanoslit, it can be efficiently channeled into a high-purity nanoslit mode within a waveguiding length <10 μm. The CNP can be either freestanding or on-chip by using a tapered fiber or planar waveguide for input-coupling, with a coupling efficiency up to 95%. Within the slit region, the output diffraction-limited nanoslit mode offers an extremely confined optical field (∼0.3 nm × 3.3 nm) with a peak-to-background ratio higher than 25 dB and can be operated within a 200-nm bandwidth. The group velocity dispersion of the nanoslit mode for ultrafast pulsed operation is also briefly investigated. Compared with the previous lasing configuration, the waveguiding scheme demonstrated here is not only simple and straightforward in structural design but is also much flexible and versatile in operation. Therefore, the waveguiding scheme we show here may offer an efficient and flexible platform for exploring light–matter interactions beyond the nanometer scale, and developing optical technologies ranging from superresolution nanoscopy and atom/molecule manipulation to ultra-sensitivity detection.
sub-nm confined optical field nanoslit evanescent coupling waveguide mode 
Advanced Photonics
2023, 5(4): 046003
张海波 1,2,*王传民 1马伟刚 1高华昀 1[ ... ]谭划 1,2
作者单位
摘要
1 华中科技大学材料科学与工程学院,材料成形与模具技术国家重点实验室 武汉 430074
2 广东华中科技大学工业技术研究院 广东 东莞 523808
3 华中科技大学光学与电子信息学院 武汉 430074
挠曲电效应是一种应变梯度与电极化(正挠曲电效应)或电场强度梯度与应变(逆挠曲电效应)之间的力电耦合效应。与压电效应不同,挠曲电效应不受材料对称性、Curie温度所限制,且随着材料尺寸减小而不断增强,因而具有广阔的研究与应用前景。本文主要总结了挠曲电效应的发展历史、挠曲电系数测量、挠曲电效应增强机制以及当前研究进展,重点介绍了挠曲电效应在传感器、致动器、机械存储器、挠曲电压电复合材料、俘能器以及新型电子器件等领域应用的最新研究进展,最后对挠曲电效应的发展前景进行了展望。
挠曲电效应 压电效应 机电耦合 应变梯度 flexoelectric effect piezoelectric effect mechanical-electric coupling strain gradient 
硅酸盐学报
2023, 51(3): 812
作者单位
摘要
中国船舶科学研究中心,江苏 无锡 214082
针对船舶舱内复杂空间材料表面除锈需求,利用脉冲光纤激光清洗平台开展了EH36船用钢板激光清洗工艺参数优化与清洗后材料表面性能实验研究。通过宏观、微观形貌观测与表面化学成分分析,并结合船舶行业除锈标准规范,建立了船用钢激光除锈质量评价准则,以此确定了材料激光除锈最佳工艺参数。在此基础上开展激光除锈后材料表面质量、显微硬度、粗糙度及综合力学性能测试评估。研究结果表明:在最佳除锈工艺参数(平均功率210 W、重复频率250 kHz、脉冲宽度300 ns、扫描速度4000 mm/s)下,船用钢板表面质量达到Sa2.5等级,力学性能基本保持不变,能够满足船舶舱内复杂空间材料表面除锈工艺要求,在船舶修造材料表面除锈领域具有优良的适用性。
激光除锈 船舶建造 工艺参数 性能评估 表面质量 laser derusting shipbuilding process parameters performance evaluation surface quality 
红外与激光工程
2023, 52(2): 20220155

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