4-nJ铒全光纤混合高啁啾耗散孤子振荡器

I. Zhdanov, D. Kharenko, A. Bednyakova, M. Fedoruk, S. Turitsyn, S. Babin
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引用次数: 0

摘要

在1550nm波长具有高脉冲能量的超快光纤激光器对于一系列应用非常重要:从CARS[1],少周期脉冲产生[2]和频率计量到太赫兹波产生。这些应用不仅需要高脉冲能量,而且需要短持续时间和高发电稳定性。非线性极化演化(NPE)效应驱动的高啁啾(啁啾参数> 10)耗散孤子生成技术(HCDS)满足上述要求。先前在含有偏振维持(PM)和非PM部件的yb光纤全光纤NPE锁模腔中获得了大量的HCDS能量增加[3]。我们在[4]中首次在1.5微米波长区域实现了这种方法,展示了165 fs解密持续时间和0.93 nJ能量的HCDS。我们还观察到由NPE超速引起的多脉冲产生机制。在这项工作中,我们扩展了我们的结果,并通过显着延长全光纤腔来增加单HCDS能量。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
4-nJ Erbium All-Fiber Hybrid Highly Chirped Dissipative Soliton Oscillator
Ultrafast fiber lasers with a high pulse energy at 1550 nm wavelength are important for a range of applications: from CARS [1], few-cycle pulse generation [2] and frequency metrology to THz-wave generation. These applications require not only the high pulse energy, but also short duration, and high generation stability. Highly chirped (chirp parameter > 10) dissipative soliton (HCDS) generation technique (HCDS) driven by the nonlinear polarization evolution (NPE) effect meets all the above requirements. Substantial HCDS energy increase has been obtained previously in Yb-fiber all-fiber NPE mode-locked cavity containing polarization maintaining (PM) and non-PM parts [3]. We have implemented this approach for 1.5 microns wavelength area for the first time in [4] demonstrating 165 fs dechirped duration and 0.93 nJ energy HCDS. We also observed a multi-pulse generation regime caused by NPE overdriving. In this work we extend our results and increase the single HCDS energy by significantly lengthening the all-fiber cavity.
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