Minghui Li 1,2Renhong Gao 1,2Chuntao Li 3,4Jianglin Guan 3,4[ ... ]Ya Cheng 1,2,3,6,7,**
Author Affiliations
Abstract
1 State Key Laboratory of High Field Laser Physics and CAS Center for Excellence in Ultra-Intense Laser Science, Shanghai Institute of Optics and Fine Mechanics (SIOM), Chinese Academy of Sciences (CAS), Shanghai 201800, China
2 Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
3 XXL—The Extreme Optoelectromechanics Laboratory, School of Physics and Electronic Science, East China Normal University, Shanghai 200241, China
4 State Key Laboratory of Precision Spectroscopy, East China Normal University, Shanghai 200062, China
5 School of Physical Science and Technology, ShanghaiTech University, Shanghai 200031, China
6 Shanghai Research Center for Quantum Sciences, Shanghai 201315, China
7 Hefei National Laboratory, Hefei 230088, China
We demonstrate single-mode microdisk lasers in the telecom band with ultralow thresholds on erbium-ytterbium co-doped thin-film lithium niobate (TFLN). The active microdisk was fabricated with high-Q factors by photolithography-assisted chemomechanical etching. Thanks to the erbium-ytterbium co-doping providing high optical gain, the ultralow loss nanostructuring, and the excitation of high-Q coherent polygon modes, which suppresses multimode lasing and allows high spatial mode overlap between pump and lasing modes, single-mode laser emission operating at 1530 nm wavelength was observed with an ultralow threshold, under a 980-nm-band optical pump. The threshold was measured as low as 1 µW, which is one order of magnitude smaller than the best results previously reported in single-mode active TFLN microlasers. The conversion efficiency reaches 4.06 × 10-3, which is also the highest value reported in single-mode active TFLN microlasers.
lithium niobate microcavities microdisk lasers 
Chinese Optics Letters
2024, 22(4): 041301
Renhong Gao 1,6Ni Yao 2Jianglin Guan 3,4Li Deng 3,4[ ... ]Ya Cheng 1,3,4,6,7,8,9,**
Author Affiliations
Abstract
1 State Key Laboratory of High Field Laser Physics and CAS Center for Excellence in Ultra-Intense Laser Science, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences (CAS), Shanghai 201800, China
2 Research Center for Intelligent Sensing, Zhejiang Lab, Hangzhou 311100, China
3 XXL—The Extreme Optoelectromechanics Laboratory, School of Physics and Electronic Science, East China Normal University, Shanghai 200241, China
4 State Key Laboratory of Precision Spectroscopy, East China Normal University, Shanghai 200062, China
5 State Key Laboratory of Modern Optical Instrumentation, College of Optical Science and Engineering, Zhejiang University, Hangzhou 310027, China
6 Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
7 Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan 030006, China
8 Collaborative Innovation Center of Light Manipulations and Applications, Shandong Normal University, Jinan 250358, China
9 Shanghai Research Center for Quantum Sciences, Shanghai 201315, China
We demonstrate integrated lithium niobate (LN) microring resonators with Q factors close to the intrinsic material absorption limit of LN. The microrings are fabricated on pristine LN thin-film wafers thinned from LN bulk via chemo-mechanical etching without ion slicing and ion etching. A record-high Q factor up to 108 at the wavelength of 1550 nm is achieved because of the ultra-smooth interface of the microrings and the absence of ion-induced lattice damage, indicating an ultra-low waveguide propagation loss of 0.0034 dB/cm. The ultra-high Q microrings will pave the way for integrated quantum light source, frequency comb generation, and nonlinear optical processes.
lithium niobate microcavities waveguide 
Chinese Optics Letters
2022, 20(1): 011902
邓莉 *
作者单位
摘要
桂林航天工业学院 广西高校无人机遥测重点实验室, 广西 桂林 541004
针对暗原色先验去雾算法对明亮区域失效, 以及分块求取暗原色存在的块状效应、Halo现象和运算复杂度较高等问题, 提出了一种基于自适应参数的全局暗原色先验去雾算法。该算法采用全局暗原色操作取代分块处理, 并通过模糊逻辑控制器自适应估计明亮区域的容差参数和透射率调整因子; 在非明亮区域求取大气光强度后, 根据自适应容差纠正明亮区域被错误估计的透射率。与常用的3种图像复原去雾算法进行了比较, 结果表明: 该算法去雾图像的主观视觉效果较好, 且图像对比度、信息熵和平均梯度3方面的客观评价结果也明显优于其它3种对比算法。该算法可有效解决明亮区域失真和分块处理带来的上述问题, 在不增加曝光处理情况下也能获得较好的去雾效果, 运算效率也有较大提升。
图像去雾 全局暗原色先验 模糊逻辑控制 明亮区域 自适应容差 image dehazing global dark channel prior fuzzy logic control bright area adaptive tolerance 
光学 精密工程
2016, 24(4): 892
作者单位
摘要
中国地震局地震预测研究所, 北京100036
常温、 1.0~4.4GPa下, 利用激光拉曼光谱研究了奥长石晶体结构随压力的变化。 发现, 压力为2.9 GPa时, 517 cm-1附近出现新的谱峰, 奥长石开始相变。 3.4 GPa时, 源于奥长石结构中M—O伸缩振动的288 cm-1拉曼谱峰频移发生突变, 517 cm-1附近谱峰消失, 奥长石由三斜晶系完全相变为单斜晶系(P1-I1)。随压力增加, 归属于奥长石四面体结构中Si—O—Si弯曲振动的458 及516 cm-1谱峰随压力增加有规律地向高频方向偏移, 斜率分别是1.667 cm-1/GPa和3.560 cm-1/GPa, 而源于Al—O—Al弯曲振动的480 cm-1谱峰与压力没有明显的线性变化关系。 卸压过程中, 288 cm-1拉曼谱峰频移保持不变, 458, 480及516 cm-1谱峰向低频偏移。 长石类矿物的相变压力与结构中八元环所含阳离子种类有关。
奥长石 拉曼光谱 压力 相变 阳离子 Oligoclase Raman spectroscopy Pressure Phase transition Cation 
光谱学与光谱分析
2012, 32(3): 691
作者单位
摘要
华东师范大学教育部光谱学与波谱学重点实验室,华东师范大学物理系,上海 200062
采用基于遗传算法(Genetic algorithm)的自适应反馈系统,成功实现了二溴甲烷多个拉曼振动模式的选择激发。通过脉冲分析方法(二次谐波频率分辨光谱开关和二次谐波交叉频率分辨光谱开关)(SHG-FROG和SHG-XFROG),在时域和频域上对优化脉冲进行还原和分析,结果表明:空间光学调制器(SLM)将优化脉冲调制成具有负啾啁特性的脉冲串。该选择激发实验的成功实现验证了相干控制自适应系统在研究复杂分子系统方面具有良好的应用前景。
量子光学 选择增强 自适应反馈控制 相干反斯托克斯拉曼光谱 quantum optics selective enhancement adaptive feedback control coherent antiStokes Raman scattering 
量子电子学报
2007, 24(6): 0694
Author Affiliations
Abstract
Key Laboratory of Optical and Magnetic Resonance Spectroscopy (East China Normal University), Ministry of Education, and Department of Physics, East China Normal University, Shanghai 200062
The dynamics of the femtosecond pulse propagation in a plasma channel is investigated by the pump-probe longitudinal diffractometry and second harmonic generation frequency-resolved optical gating (SHG-FROG) technique. The spatial characteristics, corresponding to the electronic density and the size of the channel, can be observed by the recorded ring pattern, and the spectral and temporal characteristics are recorded by the SHG-FROG traces. The spatiotemporal characteristics will help us to better understand the dynamics of the plasma induced by the femtosecond pulse and the femtosecond pulse propagating in the plasma channel.
等离子体 自聚焦 自相位调制 有质动力 350.5400 Plasmas 320.2250 Femtosecond phenomena 060.5060 Phase modulation 190.2640 Frequency shifting 
Chinese Optics Letters
2006, 4(10): 617
作者单位
摘要
在不同刚性的聚合物基体聚甲基丙烯酸甲酯(PMMA)、聚乙烯咔唑(PVK)和聚苯乙烯(PS)薄膜基体中掺入相同质量分数(均为0.003)的分散红13(DR13)偶氮染料。以线偏振连续Ar+激光(514 nm)作为控制光,连续HeNe激光(632.8 nm)作为信号光考察了具有相同厚度的三种样品在相同控制光功率(15 mW)下的光致双折射效应。实验发现刚性较大的聚乙烯咔唑基体样品的双折射效应最小,刚性最小的聚苯乙烯基体样品的双折射效应最大。在偶氮生色团光致异构的四能级模型基础上,建立一新的唯象的模型。在模型中引入描述聚合物基体刚性的参量s,通过数值计算描述了不同基体刚性参量s对偶氮生色团光致异构取向的影响。计算结果表明,基体的刚性越大,样品的光致双折射效应越小,定性地解释了实验现象。
非线性光学 偶氮生色团 光致异构 光致双折射 唯象模拟 
光学学报
2005, 25(10): 1385
作者单位
摘要
1 中山大学光电材料与技术国家重点实验室,广州 510275
2 中山大学高分子研究所, 广州 510275
采用超快激光光谱技术研究了一种新型的卟啉侧链聚合物(HTPP-PGMA)的激发态动力学过程.研究结果表明:HTPP-PGMA的荧光弛豫过程远快于通常的小分子卟啉单体化合物的荧光弛豫过程.在近共振波长(λ=532 nm)处,观察到了HTPP-PGMA的瞬态无腔光学双稳态的响应过程.通过采用电荷转移模型对HTPP-PGMA的超快激发态动力学过程进行了分析.
中国激光
2004, 31(s1): 140
作者单位
摘要
中山大学理工学院光电材料国家重点实验室,广州,510275
介绍了一种用于超高速行波电吸收调制器(TW-EAM)设计的"k值带宽法".该方法考虑了影响调制器带宽的阻抗失配、相速度失配、微波衰减等因素,说明一个优化设计的TW-EAM其带宽可达到140 GHz.
行波电吸收调制器(TW-EAM) 调制带宽 共面波导 
光子学报
2004, 33(7): 806
作者单位
摘要
中山大学光电材料与技术国家重点实验室,理工学院,广东,广州,510275
从电极设计的角度对行波电吸收调制器(TW-EAM)的带宽进行分析,用一个共面波导的TW-EAM的测量数据进行设计计算演示,介绍了本设计方法的计算过程.计算演示结果与实验测量结果相吻合.文章还分析了中间电极宽度和电极间距对带宽的影响.并简单说明用它计算设计的一个GaAs/GaAlAs多量子阱(MQWS)TW-EAM获得大带宽的例子.
行波电吸收调制器(TW-EAM) 调制带宽 共面波导 traveling-wave electroabsorption modulator(TW-EAM modulation bandwidth coplanar waveguide 
红外与毫米波学报
2004, 23(4): 291

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