All-fiber mode-locking using a two concentric core fiber saturable absorber

Author(s):  
Elham Nazemosadat ◽  
Arash Mafi
2020 ◽  
pp. 2001821
Author(s):  
Safayet Ahmed ◽  
Junpeng Qiao ◽  
Ping Kwong Cheng ◽  
Ahmed Mortuza Saleque ◽  
Mohammad Ismail Hossain ◽  
...  

2018 ◽  
Vol 57 (24) ◽  
pp. 6937 ◽  
Author(s):  
H. Ahmad ◽  
S. A. Reduan ◽  
S. I. Ooi ◽  
M. A. Ismail

2017 ◽  
Vol 49 (11) ◽  
Author(s):  
Yung Hsu ◽  
Chien-Hung Yeh ◽  
Chi-Wai Chow

2010 ◽  
Vol 7 (3) ◽  
pp. 198-202 ◽  
Author(s):  
J.-L. Xu ◽  
J.-L. He ◽  
H.-T. Huang ◽  
J.-F. Yang ◽  
B.-T. Zhang ◽  
...  

1998 ◽  
Vol 47 (1) ◽  
pp. 9
Author(s):  
HUANG ZHI-JIAN ◽  
SUN JUN-QIANG ◽  
HUANG DE-XIU

1998 ◽  
Author(s):  
Vladimir L. Kalashnikov ◽  
D. O. Krimer ◽  
Igor G. Poloyko ◽  
Victor P. Mikhailov

2020 ◽  
Vol 10 (1) ◽  
Author(s):  
Masayuki Suzuki ◽  
Ozdal Boyraz ◽  
Hossein Asghari ◽  
Bahram Jalali

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.


2019 ◽  
pp. 401-430
Author(s):  
Anas Abdul Latiff ◽  
Anas Abdul Latiff ◽  
Sulaiman Wadi Harun ◽  
Muhammad Farid Mohd Rusdi ◽  
Harith Ahmad

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