Generation of broadband continuous-wave supercontinuum Raman lasing in a fiber ring cavity

2006 ◽  
Author(s):  
Wei Zhang ◽  
Yan Wang ◽  
Li Xiao ◽  
Jiangde Peng
2019 ◽  
Vol 33 (09) ◽  
pp. 1950076 ◽  
Author(s):  
Min Luo ◽  
Wei Cao ◽  
Haiyan Chen

The effect of semiconductor saturable absorber mirror (SESAM) on continuous-wave multi-wavelength fiber ring-cavity laser with semiconductor optical amplifier (SOA) is experimentally demonstrated. The evolutionary process of multi-wavelength oscillation and the decrease of oscillating mode number caused by an SESAM are discussed. It’s found that the free oscillating mode number of the multi-wavelength fiber ring-cavity laser with SOA can be upto three, and the lasing wavelengths are 1573.8 nm, 1578.09 nm and 1582.37 nm, respectively. When a SESAM is inserted in the fiber ring-cavity, it narrows the amplified spontaneous emission (ASE) spectrum of the SOA, and the oscillating mode number of the multi-wavelength fiber ring-cavity lasers with SOA decreases to two, a stable dual-wavelength lasing at 1560.91 nm and 1564.12 nm is obtained.


2020 ◽  
pp. 1-1
Author(s):  
Yunkun Zhao ◽  
Chenchen Wang ◽  
Yuanyang Zhao ◽  
Desheng Zhu ◽  
Liang Lu

Author(s):  
Abdelkrim Bendahmane ◽  
Davide Ceoldo ◽  
Julien Fatome ◽  
Guy Millot ◽  
Tobias Hansson ◽  
...  

2021 ◽  
Vol 11 (1) ◽  
pp. 407
Author(s):  
Jinho Lee ◽  
Ju Han Lee

This study reports a Q-switching-based, 2058-nm holmium (Ho) fiber laser incorporating a saturable absorber (SA) based on graphene oxide (GO). The SA was prepared with a side-polished fiber, while GO particles were deposited onto the fiber-polished surface to realize an all-fiber SA. A continuous-wave thulium-doped all-fiber laser, which was configured with a master-oscillator power-amplifier (MOPA) structure, was constructed as a pumping source. By inserting the fabricated SA into an all-fiber ring resonator based on 1-m length of Ho-doped fiber, Q-switched pulses could readily be obtained at a wavelength of 2058 nm. The pulse width was observed to vary from 2.01 to 1.56 μs as the pump power was adjusted from ~759 to 1072 mW, while the repetition rate was tunable from 45.56 to 56.12 kHz. The maximum values of average optical power and pulse energy were measured as ~11.61 mW and 207.05 nJ, respectively, at a ~1072 mW pump power.


2017 ◽  
Vol 42 (3) ◽  
pp. 435 ◽  
Author(s):  
F. Copie ◽  
M. Conforti ◽  
A. Kudlinski ◽  
S. Trillo ◽  
A. Mussot
Keyword(s):  

2016 ◽  
Vol 28 (8) ◽  
pp. 923-926 ◽  
Author(s):  
Chunran Sun ◽  
Muguang Wang ◽  
Jingxuan Liu ◽  
Shen Ye ◽  
Linjun Liang ◽  
...  

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