Yuxi Pang 1,2Qiang Ji 1,2Shaonian Ma 1,2Xian Zhao 1,2[ ... ]Yanping Xu 1,2,*
Author Affiliations
Abstract
1 Shandong University, Center for Optics Research and Engineering, Qingdao, China
2 Shandong University, Key Laboratory of Laser and Infrared System of the Ministry of Education, Qingdao, China
3 Shandong University, School of Information Science and Engineering, Qingdao, China
4 National Research Council Canada, Ottawa, Canada
5 University of Ottawa, Physics Department, Ottawa, Canada
The optical rogue wave (RW), known as a short-lived extraordinarily high amplitude dynamics phenomenon with small appearing probabilities, plays an important role in revealing and understanding the fundamental physics of nonlinear wave propagations in optical systems. The random fiber laser (RFL), featured with cavity-free and “modeless” structure, has opened up new avenues for fundamental physics research and potential practical applications combining nonlinear optics and laser physics. Here, the extreme event of optical RW induced by noise-driven modulation instability that interacts with the cascaded stimulated Brillouin scattering, the quasi-phase-matched four-wave mixing as well as the random mode resonance process is observed in a Brillouin random fiber laser comb (BRFLC). Temporal and statistical characteristics of the RWs concerning their emergence and evolution are experimentally explored and analyzed. Specifically, temporally localized structures with high intensities including chair-like pulses with a sharp leading edge followed by a trailing plateau appear frequently in the BRFLC output, which can evolve to chair-like RW pulses with adjustable pulse duration and amplitude under controlled conditions. This investigation provides a deep insight into the extreme event of RWs and paves the way for RW manipulation for its generation and elimination in RFLs through adapted laser configuration.
optical rogue wave modulation instability random fiber laser cascaded stimulated Brillouin scattering four-wave mixing temporally localized structure 
Advanced Photonics Nexus
2024, 3(2): 026008
作者单位
摘要
上海大学物理系,上海 200444
原子玻色-爱因斯坦凝聚体的调制稳定性决定了凝聚体的超流属性,是超冷原子物理研究的重要内容。在由拉曼光形成的自旋轨道耦合的玻色-爱因斯坦凝聚体中,存在4种不同的零动量本征态,由于自旋轨道耦合的存在,其中两种态载有流,另两种态不载流。通过对它们进行调制稳定性分析,发现无论在什么参数空间,这4种态都是调制不稳定的,即自旋轨道耦合总是能够诱导出调制不稳定性。这些态的动力学演化揭示调制不稳定性能够产生复杂的图案。
原子与分子物理学 自旋轨道耦合 玻色-爱因斯坦凝聚体 调制不稳定性 
光学学报
2023, 43(21): 2102001
Author Affiliations
Abstract
1 University of Technology and Applied Sciences, P.O. Box 14, Ibri 516, Oman
2 Department of Mathematics, Sultan Qaboos University, P.O.Box 36, Al-Khod 123, Muscat, Oman
3 Department of Mathematics and Physics, Grambling State University, Grambling, LA 71245, USA
4 Mathematical Modeling and Applied Computation (MMAC) Research Group, Department of Mathematics, King Abdulaziz University, Jeddah 21589, Saudi Arabia
5 Department of Applied Mathematics, National Research Nuclear University, 31 Kashirskoe Hwy, Moscow 115409, Russian Federation
6 Department of Applied Sciences, Cross-Border Faculty, Dunarea de Jos University of Galati, 111 Domneasca Street, Galati 800201, Romania
7 Department of Mathematics and Applied Mathematics, Sefako Makgatho Health Sciences University, Medunsa 0204, Pretoria, South Africa
The objective of this study is to investigate miscellaneous wave structures for perturbed Fokas–Lenells equation (FLE) with cubic-quartic dispersion in polarization-preserving fibers. Based on the improved projective Riccati equations method, various types of soliton solutions such as bright soliton, combo dark–bright soliton, singular soliton and combo singular soliton are constructed. Additionally, a set of periodic singular waves are also retrieved. The dynamical behaviors of some obtained solutions are depicted to provide a key to understanding the physics of the model. The modulation instability of the FLE is reported by employing the linear stability analysis which shows that all solutions are stable.The objective of this study is to investigate miscellaneous wave structures for perturbed Fokas–Lenells equation (FLE) with cubic-quartic dispersion in polarization-preserving fibers. Based on the improved projective Riccati equations method, various types of soliton solutions such as bright soliton, combo dark–bright soliton, singular soliton and combo singular soliton are constructed. Additionally, a set of periodic singular waves are also retrieved. The dynamical behaviors of some obtained solutions are depicted to provide a key to understanding the physics of the model. The modulation instability of the FLE is reported by employing the linear stability analysis which shows that all solutions are stable.
Perturbed Fokas–Lenells equation Optical solitons Cubic-quartic dispersion Improved projective Riccati equations method Modulation instability 
Journal of the European Optical Society-Rapid Publications
2022, 18(2): 2022008
作者单位
摘要
国防科技大学 气象海洋学院深海科学与技术实验室, 长沙 410073
随着远程光纤水听器系统传输距离的不断扩展, 各类光学非线性效应的影响日益凸显, 并已成为制约远程光纤水听器系统性能的瓶颈。回顾了远程光纤水听器系统中光学非线性效应研究进展, 对系统中存在的光学非线性效应进行分析, 并重点介绍了系统中受激布里渊散射与调制不稳定性的产生机理及其对系统相位噪声的影响, 并介绍相应的抑制方法。
光纤水听器 受激布里渊散射 调制不稳定性 optical fiber hydrophone stimulated Brillouin scattering modulation instability 
半导体光电
2022, 43(4): 738
作者单位
摘要
1 山西大学 理论物理研究所,山西 太原 030006
2 山西医科大学 物理教研室,山西 太原 030001
在色散振荡光纤中,研究平均色散、色散振荡周期和色散振荡振幅对准连续泵浦波输出调制不稳定性增益边带的影响。结果表明:随着平均色散和色散振荡周期的增加,各阶边带中心向频谱的中心频率移动,并且相对应的增益值逐渐减小。特别地,当色散振荡周期以整数增加时,在一定频谱范围内,会出现对称不等增益边带组。然而,增强色散振荡振幅,各阶边带中心频率并不发生改变,此时各阶边带增益出现振荡周期性的减小,边带出现分裂和消失的现象。同时,利用解析公式对离散增益边带进行理论预测,讨论解析公式的适用性。
色散振荡光纤 调制不稳定性 准连续泵浦波 振荡参数 增益边带 Dispersion oscillating fiber Modulation instability Quasi-continuous pump wave Oscillating parameter Gain sidebands 
量子光学学报
2017, 23(4): 372
林蓉 *
作者单位
摘要
菏泽学院 物理与电子工程系, 山东 菏泽 274015
在非线性自散焦LiNbO3∶Fe晶体中, 实验观察了用激光作光源和用白光作光源两种情况下所产生的调制不稳定性, 并从三个方面对这两种情况进行了比较。实验结果表明: 在两种情况下, 达到稳定状态前, MI现象都会随辐照时间的增加而变得越来越清晰, 并且MI图样都会随着入射光束形状的变化而变化。不同的是, 用白光作光源时, 灯丝长度方向与晶体c轴方向的夹角大于等于45°时出现MI, 而用激光作光源时, 入射光束方向与c轴方向的夹角不大于45°才出现MI。
非线性光学 调制不稳定性(MI: modulation instability) LiNbO3∶Fe晶体 自散焦介质 nonlinear optics modulation instability(MI) LiNbO3∶Fe crystal self-defocusing media 
光学技术
2017, 43(5): 434
作者单位
摘要
北京工业大学激光工程研究院, 北京 100124
采用在谐振腔内加入非线性介质的方法,制作了由谐振腔直接产生超连续谱输出的全光纤结构激光器。解决了传统超连续谱激光器光源需要高功率和多级放大结构的问题。利用声光调制器作为调Q 介质,在调制不稳定性效应的影响下使脉冲分裂,利用谐振腔直接输出的结构获得了平均功率为102 mW 的超连续谱输出,光谱范围为440~1700 nm,10 dB带宽为500 nm,光-光转换效率为5%。
激光器 超连续谱 谐振腔 调制不稳定性 
中国激光
2016, 43(2): 0202005
林蓉 *
作者单位
摘要
菏泽学院 物理与电子工程系,山东 菏泽 274015
在LiNbO3∶Fe晶体中实验观察了由内在噪音引起的调制不稳定性和加入振幅掩模后产生的调制不稳定性,并对二者进行了比较。在使用振幅掩模时,根据晶体c轴方向与振幅掩模所带周期格子暗斑主轴方向的关系,分两种配置进行了观察比较,第一种配置是二者平行,第二种配置是二者成45°夹角。实验结果表明,掩模的加入加快了调制不稳定性的出现,但在第二种配置下产生的调制不稳定性对晶体内已形成的光子晶格的影响较小,并且这些周期性的光子晶格反过来对调制不稳定性的进一步发展有很好地抑制作用。由于光孤子有很高的应用价值,而调制不稳定性被看作是光孤子形成的预兆,所以研究它具有广泛的应用前景。
非线性光学 调制不稳定性 自散焦介质 晶体 nonlinear optics modulation instability self-defocusing media LiNbO3∶Fe crysta 
光学技术
2015, 41(4): 301
作者单位
摘要
郑州华信学院 信息工程系,河南 新郑 451150
应用Compton散射模型和非线性Schrdinger方程,研究了Compton散射对等离子体零色散附近调制不稳定性的影响,提出了将Compton散射作为形成调制不稳定性的新机制,给出了等离子体修正色散方程,并进行了数值计算.结果表明:二阶色散较大时,远离零色散附近调制不稳定性增益谱由入射和散射光产生的二阶色散决定,随二阶色散增大,四阶色散作用迅速减小,这是因散射效应有效削弱了四阶效应的缘故.零色散附近调制不稳定性增益谱由入射和散射光产生的四阶色散决定,二阶色散被湮灭,微扰频率最大值向临界微扰频率较快靠近,这是因散射效应有效增强了四阶效应的缘故.增益谱宽随等离子体损耗增大而迅速增大,这是因功率增大使散射效应增强,导致带电粒子辐射阻尼增强的缘故.
等离子体 非线性光学 数值计算 调制不稳定性 色散 耦合 多光子非线性Compton散射 Plasma Nonlinear optics Numerical computing Modulation instability Dispersion Coupling Multi-photon nonlinear Compton scattering 
光子学报
2014, 43(10): 1019002
作者单位
摘要
1 湖南商学院计算机与信息工程学院, 湖南 长沙 410205
2 华中科技大学光学与电子信息学院, 湖北 武汉 430074
在考虑线性损耗的情况下,对硅基纳米波导中皮秒脉冲传输交叉相位调制不稳定性进行了仿真研究。采用微扰和线性稳定性分析方法,理论推导了调制不稳定性产生所满足的色散关系和调制不稳定性增益谱表达式。分析了脉冲光功率、线性损耗和群速度色散系数等参量对交叉相位调制不稳定性的影响,并进行了仿真分析。结果表明,即使在微弱的入射光功率下,仍然存在强烈的交叉相位调制不稳定性现象;交叉相位调制不稳定性不仅可以在反常色散区出现,而且在正常色散区也会发生。波导的线性损耗对交叉相位调制不稳定性增益谱有明显影响。
非线性光学 交叉相位调制不稳定性 线性损耗 硅基纳米波导 nonlinear optics cross-phase modulation instability linear loss silicon nanometer waveguide 
光学与光电技术
2014, 12(4): 31

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