作者单位
摘要
1 浙江师范大学物理与电子信息工程学院,浙江 金华 321004
2 浙江省光信息检测与显示技术研究重点实验室,浙江 金华 321004
提出一种环形相位构造方法,并通过实验产生了一种可调谐手性结构光场。在螺旋相位的基础上引入径向相位与等相相位形成环形子相位,在平面波上加载该相位产生单环手性结构光场。进一步利用相位叠加原理,组合多个不同环形子相位构成一个环形相位,进而利用其调控产生多环形手性结构光场。研究发现,通过控制拓扑荷数、等相位因子、径向偏移因子,能够灵活控制螺旋强度瓣叶的数量以及手性方向。此外,通过引入等相位梯度实现了光场的动态旋转。所构建的可调谐手性结构光场有益于手性结构微加工,在光学微操纵及光学通信领域也有较大的潜在应用价值。
物理光学 光场调控 相位调制 结构光场 手性光场 
光学学报
2024, 44(8): 0826002
Author Affiliations
Abstract
National Key Laboratory of Tunable Laser Technology, Institute of Opto-Electronics, Harbin Institute of Technology, Harbin 150080, China
Fast and stable phase control is essential for many applications in optics. Here, we propose an all-fiber all-optical phase modulation scheme based on a Fabry–Perot interferometer (FPI) and an Er/Yb co-doped fiber (EYDF). By using the EYDF as an F-P cavity via rational design, a phase shift with a modulation sensitivity of 0.0312π/mW is introduced to the modulator. The phase shifts in the EYDF consist of a thermal phase shift and a nonlinear phase shift with a ratio of 19:1, and the corresponding temporal responses of the modulation are 204 ms and 2.5 ms, respectively. In addition, the compact FPI is encapsulated to provide excellent stability for the modulator.
in-line Fabry-Perot interferometer nonlinear phase shift all-optical phase modulation 
Chinese Optics Letters
2024, 22(4): 041901
Author Affiliations
Abstract
1 SwissFEL, Paul Scherrer Institute, Villigen PSI, Switzerland
2 Photonics Institute, Technische Universität Wien, Vienna, Austria
3 Institute of Applied Physics, University of Bern, Bern, Switzerland
4 Institute for Quantum Electronics, Physics Department, ETH Zurich, Zurich, Switzerland
We demonstrate the generation, spectral broadening and post-compression of second harmonic pulses using a thin beta barium borate (BBO) crystal on a fused-silica substrate as the nonlinear interaction medium. By combining second harmonic generation in the BBO crystal with self-phase modulation in the fused-silica substrate, we efficiently generate millijoule-level broadband violet pulses from a single optical component. The second harmonic spectrum covers a range from long wave ultraviolet (down to 310 nm) to visible (up to 550 nm) with a bandwidth of 65 nm. Subsequently, we compress the second harmonic beam to a duration of 4.8 fs with a pulse energy of 0.64 mJ (5 fs with a pulse energy of 1.05 mJ) using chirped mirrors. The all-solid free-space apparatus is compact, robust and pulse energy scalable, making it highly advantageous for generating intense second harmonic pulses from near-infrared femtosecond lasers in the sub-5 fs regime.
post-compression second harmonic generation self-phase modulation supercontinuum generation 
High Power Laser Science and Engineering
2024, 12(2): 02000e16
董一甲 1,2刘杰 1赵欣瑞 1,2林星辰 1[ ... ]朱洪波 1,*
作者单位
摘要
1 中国科学院长春光学精密机械与物理研究所,吉林 长春 130033
2 中国科学院大学,北京 100049
采用具有模式转换和无损传输特性的三模非模式选择光子灯笼(PL)实现了976 nm波长的半导体激光的相干合束。相对于半导体激光常规空间孔径相干合束的方式,所提合束光场不会产生旁瓣,且能拥有较高的光束质量。通过仿真PL合束特性,搭建合束实验系统,最终976 nm波长的半导体激光基模输出功率达99.7 mW,转换效率为33.2%。实验结果表明,此合束系统实现了模式转换,使半导体激光能够以基模输出,展现了一种有潜力的半导体激光相干合束的方法。
半导体激光 光子灯笼 相干合束 相位调控 光纤模式 
激光与光电子学进展
2024, 61(5): 0514006
作者单位
摘要
1 西安工业大学光电工程学院,陕西 西安 710021
2 中国科学院西安光学精密机械研究所光子制造系统与应用研究中心,陕西 西安 710119
液晶空间光调制器(LCSLM)加载计算全息图实现激光分束时,会在焦平面处产生零级光干扰,为了解决这一情况,提出一种加载达曼光栅灰度图至液晶空间光调制器的方法,利用相消干涉,从而消除零级光干扰。基于模拟退火算法,求解出相位转折点集,在VirtualLab中进行仿真模拟,利用MATLAB软件编写生成达曼光栅灰度图的脚本文件,搭建基于硅基液晶空间光调制器(LCOSSLM)的验证系统,对调制效果进行测验。结果表明:通过加载达曼光栅灰度图进行激光分束,在CCD视场内明显去除了零级光干扰,且实际分束效果与仿真模拟结果相近,在一维五分束下的分束均匀度达97.190%,优于GSW算法生成的光栅形式全息图的调制效果。以大光点间距进行一维二、七分束的效果观测,分束均匀度分别达98.453%、96.820%,又进行二维分束观测,测量分束均匀度可达95.436%,且均未在CCD视场内观测到零级光。
液晶空间光调制器 飞秒激光 纯相位调制 达曼光栅 衍射结构 
激光与光电子学进展
2024, 61(4): 0411008
Author Affiliations
Abstract
1 Instituto de Bioingeniería, Universidad Miguel Hernández, Elche 03202, Spain
2 Departamento de Física Aplicada, Universidad Miguel Hernández, Elche 03202, Spain
3 Departamento de Ciencia de Materiales, Óptica y Tec. Electrónica, Universidad Miguel Hernández, Elche 03202, Spain
In this work, we compare different methods for implementing a triplicator, a phase grating that generates three equi-intense diffraction orders. The design with optimal efficiency features a continuous phase profile, which cannot be easily reproduced, and is typically affected by quantization. We compare its performance with binary and sinusoidal phase profiles. We also analyze the effect of quantizing the phase levels. Finally, a random approach is adopted to eliminate the additional harmonic orders. In all cases, a liquid-crystal-on-silicon spatial light modulator is employed to experimentally verify and compare the different approaches.
diffraction gratings phase modulation triplicator spatial light modulators 
Chinese Optics Letters
2024, 22(2): 020501
Author Affiliations
Abstract
1 Key Laboratory of High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai, China
2 Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, China
Frequency modulation (FM)-to-amplitude modulation (AM) conversion is an important factor that affects the time–power curve of inertial confinement fusion (ICF) high-power laser facilities. This conversion can impact uniform compression and increase the risk of damage to optics. However, the dispersive grating used in the smoothing by spectral dispersion technology will introduce a temporal delay and can spatially smooth the target. The combined effect of the dispersive grating and the focusing lens is equivalent to a Gaussian low-pass filter, which is equivalent to 8 GHz bandwidth and can reduce the intensity modulation on the target to below 5% with 0.3 nm @ 3 GHz + 20 GHz spectrum phase modulation. The results play an important role in the testing and evaluating of the FM-to-AM on the final optics and the target, which is beneficial for comprehensively evaluating the load capacity of the facility and isentropic compression experiment for ICF.
dispersion grating frequency modulation-to-amplitude modulation conversion high-power laser facility inertial confinement fusion phase modulation 
High Power Laser Science and Engineering
2024, 12(1): 010000e9
作者单位
摘要
1 上海交通大学生物医学工程学院Med-X研究院,上海 200030
2 中国科学院苏州生物医学工程技术研究所,江苏 苏州 215163
超透镜作为一种二维超表面结构最近十多年来得到了广泛的关注。与传统光学透镜相比,超透镜具有超薄和超轻的结构特性以及高度灵活的设计和调控能力,因此,其在推动光学系统向小型化发展中扮演着不可或缺的角色。在显微成像技术中,超透镜又提供了多维度的探索视角,展示了其巨大的发展空间。本文全面回顾了超透镜在显微成像技术的最新进展。首先,详细解释了超透镜的波前调控原理,并总结了超透镜主流的设计方法;其次,介绍了超透镜的加工技术;最后,深入探讨了超透镜在光片荧光显微镜、双光子荧光显微镜和内窥镜等显微成像技术中的应用和研究进展。
超透镜 超表面 显微成像 相位调制 
激光与光电子学进展
2024, 61(2): 0211028
作者单位
摘要
1 天津大学精密仪器与光电子工程学院超快激光实验室,天津 300072
2 天津大学佐治亚理工深圳学院,广东 深圳 518055
基于掺Yb3+光纤和掺Yb3+晶体的飞秒激光器输出的飞秒激光脉冲具有较高的脉冲能量和平均功率,被广泛应用于科研和工业生产;但受Yb3+增益介质增益带宽的限制,输出脉冲宽度很难小于300 fs。利用飞秒激光脉冲在多层薄板中的自相位调制效应,分别对基于掺Yb3+光纤和掺Yb3+晶体的飞秒激光器输出的飞秒激光脉冲进行非线性压缩。通过优化非线性压缩装置的各项参数,实现了对低能量、窄脉宽和高能量、宽脉宽脉冲的非线性压缩,分别获得了脉冲能量为64 μJ、脉冲宽度为42 fs和脉冲能量为315 μJ、脉冲宽度为79 fs的飞秒激光脉冲输出,第一级非线性压缩效率均超过80%,整体压缩效率分别为53%和65%。
激光器 飞秒激光脉冲 自相位调制 非线性压缩 光谱展宽 
中国激光
2024, 51(2): 0201003
作者单位
摘要
华中科技大学 武汉光电国家研究中心, 武汉 430074
为了研究和论证锗硅材料体系在器件的工艺制备和理论性能上的优势, 拓展锗硅量子阱结构的应用范围, 采用数值仿真结合实际器件制备的方法, 进行了理论分析和实验验证, 设计了一种基于Ge/SiGe非对称耦合量子阱材料的光学相位调制器, 并在实验测试中验证了该理论的正确性。结果表明, 当电场超过40 kV/cm时, 该材料在1450 nm波长处可以达到最高0.01的电致折射率变化; 经测试发现, 实际制备的器件在1.5 V的反向偏置电压下,实现了1530 nm波长处2.4×10-3的电致折射率变化, 对应的VπLπ=0.048 V·cm, 在同类型锗硅光调制器中达到了先进水平。该研究为硅基集成光调制器的进一步发展开辟了新的方向。
集成光学 锗硅调制器 非对称耦合量子阱 相位调制 integrated optics Ge/SiGe modulator asymmetric coupled quantum well phase modulation 
激光技术
2023, 47(5): 587

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