作者单位
摘要
1 中国科学院物理研究所 光物理重点实验室,北京 100190
2 上海理工大学 光电信息与计算机工程学院,上海 200093
基于差频产生的中红外飞秒光源具有波长调谐范围宽(6~20 μm)、覆盖范围广(整个“指纹区”)和系统复杂程度低等优势,超快光纤激光器驱动的中红外飞秒光源只有差频部分采用了空间光路,进一步提高了系统的稳定性。文中介绍基于超快光纤激光器驱动的光学差频产生长波中红外飞秒脉冲的技术路线,阐述在差频过程中如何通过非线性光纤光学技术(包括超连续谱产生、孤子自频移和光谱滤波技术)产生合适的信号脉冲,并从理论上详细介绍差频过程中提高中红外脉冲功率的方法。
飞秒中红外光源 光纤激光 差频产生 非线性光纤光学技术 中红外晶体 fs mid-IR light source fiber laser difference-frequency generation nonlinear fiber optics technology mid-infrared crystal 
红外与激光工程
2021, 50(8): 20210368
张静 1,2,*程林 1,2罗传仙 1,2江翼 1,2石悠旖 1,2
作者单位
摘要
1 南瑞集团(国网电力科学研究院)有限公司,江苏 南京 211006
2 国网电力科学研究院武汉南瑞有限责任公司,湖北 武汉 430074
介绍了一种基于分离脉冲的掺铒光纤飞秒激光放大技术及光源装置。该光源采用分离脉冲放大技术将待放大种子脉冲先通过偏振复用方式分割成若干个子脉冲,再由光纤主放大器非线性放大和压缩,从而免去了光栅对或者棱镜对的使用。1.55 μm波段分离脉冲放大技术的特点在于不仅可以有效降低飞秒脉冲放大过程中的光谱非线性畸变,实现无基底的时域脉冲输出,而且可以通过管理泵浦光强度和光纤长度对非线性效应和光谱展宽程度进行精细控制。实验上,研究了主放大器在低非线性条件和高非线性条件下的脉冲放大和压缩效果。其中,在低非线性条件下,主放大器直接输出脉冲宽度830 fs,平均功率3 W的激光,相应峰值功率为36.1 kW;在高非线性条件下,主放大器直接输出脉冲宽度137 fs、平均功率1.54 W的激光,相应峰值功率为112 kW。通过周期极化铌酸锂晶体光学倍频验证了1560 nm飞秒脉冲的对比度,倍频效率最高可达40.3%。
激光技术 激光放大器 掺铒光纤 非线性光纤光学 锁模激光器 
激光与光电子学进展
2021, 58(19): 1914001
Author Affiliations
Abstract
Ultrafast Laser Laboratory, School of Precision Instrument and Optoelectronics Engineering, Key Laboratory of Optoelectronic Information Technology (Ministry of Education), Tianjin University, Tianjin300072, China
We numerically and experimentally investigate the multi-pulsing mechanism in a dispersion-managed mode-locked Yb-doped fiber laser. Multi-pulsing occurs primarily owing to the inherent filtering effect of the chirped fiber Bragg grating. The spectral filtering effect restricts the spectral broadening induced by self-phase modulation and causes extra loss, leading to a decreased pump power threshold for the multi-pulsing state. Numerical simulations show that multi-pulsing emerges at a lower pump power when the spectral filter bandwidth becomes narrower. In the experiment, the spectral width increases as the net cavity dispersion approaches zero. Pulses with wider spectral widths experience more loss from the spectral filtering effect, leading to a decreased pump power threshold for multi-pulsing. Therefore, the net cavity dispersion also has an impact on the multi-pulsing threshold. Based on this conclusion, we devise a strategy to obtain single-pulsing operation with the shortest pulse width and the highest pulse energy.
fiber optics oscillators nonlinear fiber optics ultrafast lasers 
High Power Laser Science and Engineering
2021, 9(3): 03000e46
Author Affiliations
Abstract
1 École Polytechnique Fédérale de Lausanne, Optics Laboratory, Lausanne, Switzerland
2 École Polytechnique Fédérale de Lausanne, Laboratory of Applied Photonics Devices, Lausanne, Switzerland
The performance of fiber mode-locked lasers is limited due to the high nonlinearity induced by the spatial confinement of the single-mode fiber core. To massively increase the pulse energy of the femtosecond pulses, amplification is performed outside the oscillator. Recently, spatiotemporal mode-locking has been proposed as a new path to fiber lasers. However, the beam quality was highly multimode, and the calculated threshold pulse energy (>100 nJ) for nonlinear beam self-cleaning was challenging to realize. We present an approach to reach high energy per pulse directly in the mode-locked multimode fiber oscillator with a near single-mode output beam. Our approach relies on spatial beam self-cleaning via the nonlinear Kerr effect, and we demonstrate a multimode fiber oscillator with M2 < 1.13 beam profile, up to 24 nJ energy, and sub-100 fs compressed duration. Nonlinear beam self-cleaning is verified both numerically and experimentally for the first time in a mode-locked multimode laser cavity. The reported approach is further power scalable with larger core sized fibers up to a certain level of modal dispersion and could benefit applications that require high-power ultrashort lasers with commercially available optical fibers.
fiber lasers spatiotemporally mode-locked lasers multimode nonlinear fiber optics 
Advanced Photonics
2020, 2(5): 056005
Author Affiliations
Abstract
1 Shenzhen University, Institute of Microscale Optoelectronics, Collaborative Innovation Center for Optoelectronic Science and Technology, Shenzhen Engineering Laboratory of Phosphorene and Optoelectronics, Shenzhen, China
2 Vrije Universiteit Brussel, Department of Applied Physics and Photonics, Brussels Photonics, Brussels, Belgium
3 Bulgarian Academy of Sciences, Institute of Solid State Physics, Sofia, Bulgaria
Rogue waves (RWs) are rare, extreme amplitude, localized wave packets, which have received much interest recently in different areas of physics. Fiber lasers with their abundant nonlinear dynamics provide an ideal platform to observe optical RW formation. We review recent research progress on rogue waves in fiber lasers. Basic concepts of RWs and the mechanisms of RW generation in fiber lasers are discussed, along with representative experimental and theoretical results. The measurement methods for RW identification in fiber lasers are presented and analyzed. Finally, prospects for future RW research in fiber lasers are summarized.
fiber lasers nonlinear fiber optics rogue wave 
Advanced Photonics
2020, 2(2): 024001
作者单位
摘要
华东师范大学精密光谱科学与技术国家重点实验室, 上海 200062
基于非线性放大环形镜,设计了一种全正色散掺镱光纤锁模激光器。在抽运功率为80 mW的情况下,该掺镱光纤锁模激光器可以实现平均功率为7.8 mW的稳定输出。输出激光脉冲的重复频率为9.9 MHz,中心波长为1064 nm,脉冲宽度约为18 ps,相应的光谱宽度为0.18 nm。该激光器具有结构简单、自启动、稳定性高的优点。
激光器 锁模激光器 光纤激光 掺镱激光 非线性光纤光学 
中国激光
2019, 46(5): 0508025
作者单位
摘要
山西大学物理电子工程学院, 山西 太原 030006
采用达布变换法得到了标准非线性薛定谔方程的一阶呼吸子解及其怪波极限,研究了一阶呼吸子解的动力学特性。借助达布变换的递推关系得到了非线性薛定谔方程的高阶呼吸子解,并分别研究了碰撞叠加、分离、简并和并行传输模式。当各呼吸子的频率趋于零时,得到非线性薛定谔方程怪波极限。研究结果表明,怪波幅值、凸起数以及怪波分裂后中心波峰的阶数和周围的波峰个数均与怪波阶数有关。
光纤光学 非线性光学 怪波 达布变换 呼吸子 简并 并行传输 
激光与光电子学进展
2019, 56(5): 050601
作者单位
摘要
1 天津大学精密仪器与光电子工程学院, 光电信息技术科学教育部重点实验室, 天津 300072
2 山东大学苏州研究院, 江苏 苏州 215123
对单模光纤中的孤子自频移效应进行了数值仿真和实验研究, 分析和验证了光纤和孤子脉冲的各种参数对孤子自频移的影响。利用分步傅里叶方法进行数值仿真, 发现孤子频移量随孤子脉冲峰值功率与光纤非线性系数的增加而增加, 随孤子脉冲宽度以及光纤色散的增加而减小。对2 km单模光纤中的孤子自频移效应进行实验研究, 通过调节孤子峰值功率实现了5.44~26.64 nm的连续可调谐移频, 所得结果与数值仿真结果一致。研究表明, 通过灵活调节孤子脉冲和光纤的各个参数, 可以有效地调节孤子频移量, 这为孤子自频移的多种实际应用提供了指导。
非线性光学 光孤子 孤子自频移 非线性光纤光学 分步傅里叶方法 
激光与光电子学进展
2018, 55(10): 101902
作者单位
摘要
1 哈尔滨工业大学可调谐激光技术国家重点实验室, 黑龙江 哈尔滨 150001
2 哈尔滨工业大学土木工程学院, 黑龙江 哈尔滨 150001
近些年,分布式布里渊光纤传感因具有分布式应变和温度的测量能力, 以及在结构健康监测领域的重要应用而受到广泛的研究。在多种传感方案中, 布里渊光时域分析(BOTDA)技术具有信噪比好、空间分辨率高、传感距离远等优点, 受到广泛关注。传统的BOTDA系统平均和扫频过程比较费时, 只适宜进行静态或缓慢的应变测量。通过分析BOTDA系统的分布式传感原理, 总结了限制其快速分布式传感测量的主要因素。针对这些限制因素, 综述了近期快速BOTDA系统取得的一系列的进展, 主要包括基于偏振补偿技术的快速BOTDA系统、基于光学捷变频技术的快速BOTDA系统、基于斜坡法的快速BOTDA系统、基于光学啁啾链的快速BOTDA系统、基于光学频率梳技术的快速BOTDA系统, 指出通过单一或者多个新技术组合而成的快速BOTDA系统具有更好的性能和更广阔的应用前景。
传感器 非线性光纤光学 受激布里渊散射 振动分析 
光学学报
2018, 38(3): 0328005
Author Affiliations
Abstract
Key Laboratory of Optical Fiber Sensing & Communications (Ministry of Education), University of Electronic Science and Technology of China, Chengdu, 611731, China
This paper presents a new technique for flat optical frequency comb (OFC) generation, which is based on the nonlinear process of multiple four-wave mixing (FWM) effects. The nonlinear effects are significantly enhanced by using the proposed optical feedback scheme consisting of a single mode fiber (SMF), two highly nonlinear fibers (HNLFs) with different zero dispersion wavelengths (ZDWs) and polarization beam splitters (PBSs). Simulation results illustrate its efficiency and applicability of expanding a comb to 128 coherent lines spaced by only 20 GHz within 6-dB power deviation.
Nonlinear fiber optics Nonlinear fiber optics multiple four-wave mixing multiple four-wave mixing optical feedback optical feedback phase modulation phase modulation self-phase modulation self-phase modulation 
Photonic Sensors
2016, 6(1): 85

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