Self-started dual-wavelength mode-locking with well-controlled repetition rate difference

2021 ◽  
pp. 1-1
Author(s):  
Zhengru Guo ◽  
Tingting Liu ◽  
Junsong Peng ◽  
Yuanjun Zhu ◽  
Kun Huang ◽  
...  
2017 ◽  
Vol 25 (15) ◽  
pp. 17192 ◽  
Author(s):  
Yazhou Wang ◽  
Jianfeng Li ◽  
Entao Zhang ◽  
Kundong Mo ◽  
Yanyan Wang ◽  
...  

2016 ◽  
Vol 34 (11) ◽  
pp. 2833-2837 ◽  
Author(s):  
Qiang Hao ◽  
Qingshan Zhang ◽  
Feihong Chen ◽  
Kangwen Yang ◽  
Heping Zeng

2011 ◽  
Vol 284 (24) ◽  
pp. 5719-5722 ◽  
Author(s):  
Jiang-Li Dong ◽  
Wen-Cheng Xu ◽  
Zhi-Chao Luo ◽  
Ai-Ping Luo ◽  
Hui-Yi Wang ◽  
...  

Author(s):  
Zhengru Guo ◽  
Qiang Hao ◽  
Junsong Peng ◽  
Heping Zeng

We report on environmentally stable long-cavity ultrashort erbium-doped fiber lasers, which self-start mode-locking at quite low thresholds by using spectrally filtered and phase-biased nonlinear amplifying long-loop mirrors. By employing 100-m polarization-maintaining fiber (PMF) in the nonlinear loop, the fundamental repetition rate reaches 1.84 MHz and no practical limitation is found to further decrease the repetition rate. The filter used in the long loop not only suppresses Kelly sidebands of the solitons, but also eliminates the amplified spontaneous emission which exists widely in low-repetition-rate ultrafast fiber lasers. The bandwidth of the filter is optimized by using a numerical model. The laser emits approximately 3-ps pulses with an energy of 17.4 pJ, which is further boosted to $1.5~\unicode[STIX]{x03BC}\text{J}$ by using a fiber amplifier.


2017 ◽  
Vol 31 (18) ◽  
pp. 1750206 ◽  
Author(s):  
Feifei Lu

We demonstrate the generation of harmonic mode-locking (HML) in an erbium-doped fiber laser with a microfiber-based rhenium disulfide (ReS2) saturable absorber (SA). Taking advantages of both saturable absorption and large third-order nonlinear effect of ReS2, HML pulse with 318.5 MHz repetition rate can be obtained, corresponding to 168th harmonic of fundamental repetition frequency of 1.896 MHz. When the pump power is increased gradually, the pulse interval remains constant, while the output power increases linearly. At the pump power of 450 mW, the output power is [Formula: see text]12 mW. The proposed high-repetition-rate pulse lasers would attract considerable attention due to its potential applications in soliton communications and frequency combs.


1994 ◽  
Vol 19 (23) ◽  
pp. 1985 ◽  
Author(s):  
S. Longhi ◽  
P. Laporta ◽  
S. Taccheo ◽  
O. Svelto

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