杨仕铭 1,2,3李尚远 2谭伊璇 1,3邓焕坚 1,2,3[ ... ]耿敏明 1,3
作者单位
摘要
1 广西大学 计算机与电子信息学院,南宁530004
2 清华大学 电子工程系,北京100084
3 广西多媒体通信与网络技术重点实验室,南宁530004
为减少目前微波光子领域到达角(AOA)测量易受相位、噪声等影响,实现二维平面内大范围的AOA测量,提出并实验验证了一种基于微波光子去斜接收的二维AOA估计方案。该方案接收端利用L型天线阵加入固定延迟时间的方法,可以估计一维AOA,利用该一维AOA可求解出二维AOA(俯仰角和方位角)。实验结果表明:在天线间隔为5 m,输入线性调频连续信号的信噪比为10 dB或-7.8 dB的情况下,所提方案的一维AOA的估计结果具有大范围的特点,且在-79°~74°内估计误差均小于2°,同时,计算得到的俯仰角和方位角在较大范围内都具有较高的精度。
微波光子学 去斜 二维到达角 线性调频信号 microwave photonics, de-chirping reception, two-di 
光通信技术
2023, 47(3): 0062
作者单位
摘要
1 辽宁工业大学化学与环境工程学院, 辽宁 锦州 121001
2 辽宁工业大学理学院, 辽宁 锦州 121001
为了获得高强度高次谐波光谱,提出了一种利用啁啾延迟来 调控H+2和D+2谐波辐射强度的方法。结果表明:在短脉宽激光驱动下, H+2和D+2 谐波辐射主要来自于激光下降区域。因此在激光下降区域引入啁啾小量会产生高强度谐波光谱连续 区, 并且H+2谐波辐射强度大于D+2谐波辐射强度。而在长脉宽激光驱动下, H+2和D+2谐 波辐射的贡献分别来自激光上升和下降区域,因此分别在激光上升和下降区域引入啁啾小量会获得相应的高强 度谐波光谱连续区, 但H+2谐波辐射强度小于D+2谐波辐射强度。最后,选择适当的谐波平台区并通过叠加谐波可获得 脉宽为36 as的孤立脉冲。
激光物理 高次谐波 啁啾调频场 双原子分子 阿秒光源 laser physics high-order harmonic generation frequency-chirping pulse diatomic molecule attosecond light sources 
量子电子学报
2020, 37(3): 314
张文飞 1,*孔伟金 2李宗文 1邢飞 1[ ... ]付圣贵 1,**
作者单位
摘要
1 山东理工大学物理与光电工程学院, 山东 淄博 255000
2 青岛大学物理科学学院, 山东 青岛 266071
超短超高能量脉冲激光作为研究光和物质相互作用的有力手段得到了广泛研究。啁啾脉冲放大系统是产生这种激光的关键部分,其中脉宽压缩光栅作为啁啾脉冲放大系统的核心组成器件,具有至关重要的作用。金属/介质膜光栅具有高衍射效率、宽工作带宽、高激光损伤阈值等优良特性,受到了广泛关注。详细综述了金属/介质膜脉宽压缩光栅的发展概况,重点分析了金属/介质膜光栅的设计原理和制作工艺,展望了金属/介质膜光栅的发展前景,旨在增进对金属/介质膜脉宽压缩光栅的了解。
光学器件 衍射光栅 多层膜 啁啾 脉宽压缩 
激光与光电子学进展
2020, 57(1): 010004
张旋 1,2王铁军 1,2,*郭豪 1,2孙海轶 1李儒新 1,2
作者单位
摘要
1 中国科学院上海光学精密机械研究所强场激光物理国家重点实验室, 上海 201800
2 中国科学院大学材料与光电研究中心, 北京 100049
研究了飞秒激光成丝过程中钳制光强对脉宽的依赖关系。对不同脉宽成丝钳制光强进行直接实验测量,发现当脉宽逐渐展宽(由45 fs展宽至177 fs)时,对应的钳制光强逐渐减小。实验结论与通过求解非线性薛定谔方程得到的数值模拟结果一致。依赖于脉宽的钳制光强的分析结果可为深入理解与脉宽相关的光丝应用提供科学依据和新思路。
激光器 飞秒现象 飞秒激光成丝 钳制光强 啁啾 
中国激光
2019, 46(9): 0901005
Author Affiliations
Abstract
School of Physics, Osnabrück University, Barbarastr. 7, 49076 Osnabrück, Germany
The role of chirp on the light–matter interaction of femto- and pico-second laser pulses with functional structured surfaces is studied using drag-reducing riblets as an example. The three-dimensional, periodic microstructure naturally gives rise to a mutual interplay of (i) reflection, (ii) scattering, and (iii) diffraction phenomena of incident coherent light. Furthermore, for femtosecond pulses, the structure induces (iv) an optical delay equivalent to a consecutive temporal delay of 230 fs in places of the pulse. These features enable studying experimentally and numerically the effect of tuning both pulse duration τ and spectral bandwidth Δω on the features of the wide-angle scattering pattern from the riblet structure. As a result, we discovered a significant breakdown of fringes in the scattering pattern with decreasing pulse duration and/or increasing spectral bandwidth. This unique type of chirp control is straightforwardly explained and verified by numerical modeling considering the spectral and temporal interaction between different segments within the scattered, linearly chirped pulse and the particular geometric features of the riblet structure. The visibility of the fringe pattern can be precisely adjusted, and the off-state is achieved using τ<230 fs or Δω>2.85×1013 rad/s.
Optical inspection Surface measurements, figure Linear and nonlinear light scattering from surfac Optical sensing and sensors Chirping Femtosecond phenomena 
Photonics Research
2018, 6(6): 06000542
作者单位
摘要
华中光电技术研究所—武汉光电国家实验室, 湖北 武汉 430223
提出了一种全光纤啁啾脉冲放大系统,在理论分析的基础上,利用分步傅里叶法,通过求解非线性薛定谔方程,对由组合A(1 m的DCF+2 m的EDF+3.08 m的SMF)与组合B(1 m的DCF+2 m的LMA-EDF+0.61 m的SMF)分别构成的两个全光纤啁啾脉冲放大系统进行分段数值模拟,结果发现,将重复频率为100 MHz、峰值功率为33.3 W、脉宽为300 fs的种子脉冲经过组合A构成的放大系统后,变为重复频率为100 MHz、峰值功率为18 062.43 W、脉宽约为56 fs的脉冲;而经过组合B构成的放大系统后,种子脉冲则变为重复频率为100 MHz、峰值功率为31 022.24 W、脉宽约为50 fs的脉冲。
啁啾脉冲放大 预啁啾 大模场面积高掺铒光纤 孤子压缩 chirped pulse amplification pri-chirping large-mode-area highly erbium-doped fiber soliton compressing 
光学与光电技术
2015, 13(3): 9
赵志龙 1,2,*苏园园 1,2吴谨 1段洪成 1,2[ ... ]黄文武 1
作者单位
摘要
1 中国科学院 电子学研究所, 北京 100190
2 中国科学院大学, 北京 100049
为解决合成孔径激光雷达(SAL)所需高重复频率大带宽相干光源问题, 提出了合成频率步进线性调频信号(SFSCS)的方案, 并进行了基于SFSCS信号SAL (SFSCS-SAL)的成像理论和实验演示研究。采用多台独立的窄带宽高重复频率线性调频激光器构成SFSCS信号, 给出了SFSCS-SAL的成像数据方程和图像形成方法。理论分析表明: 在一定条件下, SFSCS-SAL的成像处理与常规SAL相同;但是, 与单个子脉冲激光器SAL相比, SFSCS-SAL的距离向成像分辨率提高至少N倍(N为构成SFSCS的独立激光器数目)。实验演示中, 利用一台1550 nm波段的线性调波长激光器, 通过光学斩波的方法模拟生成了子脉冲数为3的SFSCS信号。以此SFSCS信号作为探测光源, 建立了SFSCS-SAL实验装置, 对强散射目标和弱散射扩展目标, 均实现了高分辨率成像。实验结果与理论分析一致。
激光雷达 合成孔径 合成线性调频步进信号 高分辨率成像 ladar synthetic aperture synthetic frequency-stepped linearly-chirping sign high resolution imaging 
强激光与粒子束
2015, 27(5): 051004
Author Affiliations
Abstract
1 College of Physics, Optoelectronics and Energy &
2 Collaborative Innovation Center of Suzhou Nano Science and Technology, Soochow University, Suzhou 215006, China
3 Research Center of Laser Fusion, China Academy of Engineering Physics, Mianyang 621900, China
We use fundamental matrix (F-matrix) method derived from coupled wave theory to simplify the diffraction simulation of chirped volume Bragg grating (CVBG) and it can be applied to arbitrary grating phase profiles. With the F-matrix method, we study the diffraction in CVBG. The spectral response of CVBG is a gate-like function, and the passband width of spectral response is related to the product of grating thickness and spatial chirp rate. The peak diffraction efficiency of CVBG increases monotonously as the amplitude of refractive index modulation increases. Incident beams with different wavelengths will be mainly diffracted at different depths of CVBG to match the Bragg condition.
090.7330 Volume gratings 050.1590 Chirping 050.1940 Diffraction 
Chinese Optics Letters
2015, 13(s1): S10901
Author Affiliations
Abstract
State Key Laboratory of Electronic Thin Films and Integrated Devices, School of Optoelectronic Information, University of Electronic Science & Technology of China, Chengdu 610054, China
A novel method for accurately measuring chromatic dispersion of optical fibers is proposed based on the use of chirped intensity-modulated signals. Unlike the conventional method, the proposed method utilizes the configurable transfer function of optical fibers caused by the residual chirp of intensity modulation, which not only eliminates the chirp error but also improves the measurement range through adjusting the chirp parameter of the intensity modulator. Our method is applicable for measuring both the magnitude and sign of chromatic dispersion of optical fibers or other dispersive devices at different operating wavelengths by using a vector network analyzer.
Radio frequency photonics Fiber measurements Dispersion Chirping 
Photonics Research
2014, 2(4): 04000B26
Author Affiliations
Abstract
We investigate the ultrafast nonlinear phenomena of picosecond chirped non-ideal hyperbolic secant pulse evolution in silicon photonic nanowire waveguides with sum frequency generation cross-correlation frequency-resolved optical gating and nonlinear Schr?dinger equation modeling. Pulse broadening and spectral blue shifts are observed experimentally, and they show remarkable agreements with numerical predictions. Nonlinear losses dominate the pulse broadening and limit the spectral bandwidth broadening induced by self-phase modulation. The initial chirp results in noticeable bandwidth compression and aggravation of blue shifts in the presence of nonlinear losses, whereas it plays a negligible role in the output pulse temporal intensity distribution.
190.7110 Ultrafast nonlinear optics 320.5390 Picosecond phenomena 320.1590 Chirping 
Chinese Optics Letters
2014, 12(s1): S11905

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