Self-Starting Harmonic Mode-Locked Thulium-Doped Fiber Laser with Carbon Nanotubes Saturable Absorber

2013 ◽  
Vol 30 (9) ◽  
pp. 094204 ◽  
Author(s):  
S. W. Harun ◽  
N. Saidin ◽  
D. I. M. Zen ◽  
N. M. Ali ◽  
H. Ahmad ◽  
...  
Author(s):  
Qianqian Huang ◽  
Chuanhang Zou ◽  
Tianxing Wang ◽  
Mohammed Al Araimi ◽  
Aleksey Rozhin ◽  
...  

Author(s):  
Qianqian Huang ◽  
Chuanhang Zou ◽  
Tianxing Wang ◽  
Chengbo Mou ◽  
Mohammed Al Araimi ◽  
...  

2018 ◽  
Vol 26 (7) ◽  
pp. 9063 ◽  
Author(s):  
Lei Hou ◽  
Hongyu Guo ◽  
Yonggang Wang ◽  
Jiang Sun ◽  
Qimeng Lin ◽  
...  

2015 ◽  
Vol 74 (8) ◽  
Author(s):  
A. A. Latiff ◽  
M. T. Ahmad ◽  
Z. Zakaria ◽  
H. Ahmad ◽  
S. W. Harun

An 1892.4 nm ultrafast passive Q-switched fiber laser is demonstrated by using Thulium-doped fiber (TDF) in conjunction with a multi-walled carbon nanotubes (MWCNTs) as a saturable absorber (SA). The MWCNTs film is sandwiched between two FC/PC fiber connectors and integrated into the laser cavity with 802 nm pump for Q-switching pulse generation. The pulse repetition rate can be tuned from 3.8 to 4.6 kHz while the corresponding pulse width reduces from 22.1 to 18.4 μs as the pump power is increased from 187.3 to 194.2 mW. A higher performance Q-switched Thulium-doped fiber laser (TDFL) is expected to be achieved with the optimization of the MWCNT-SA saturable absorber and laser cavity.


Laser Physics ◽  
2011 ◽  
Vol 21 (2) ◽  
pp. 283-286 ◽  
Author(s):  
S. M. Kobtsev ◽  
S. V. Kukarin ◽  
Y. S. Fedotov

2021 ◽  
Author(s):  
Qianqian Huang ◽  
dai lilong ◽  
Alex Rozhin ◽  
Chengbo Mou ◽  
Mohammed Al Arami

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.


2011 ◽  
Vol 19 (20) ◽  
pp. 19775 ◽  
Author(s):  
Chang Su Jun ◽  
Ju Hee Im ◽  
Sang Hwa Yoo ◽  
Sun Young Choi ◽  
Fabian Rotermund ◽  
...  

2019 ◽  
Vol 16 (2) ◽  
pp. 025103 ◽  
Author(s):  
Zhenhong Wang ◽  
Chenyang Li ◽  
Junwei Ye ◽  
Zhi Wang ◽  
Yan-Ge Liu

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