scholarly journals Experimental Study of Fiber Laser Cavity Losses to Generate a Dual-Wavelength Laser Using a Sagnac Loop Mirror Based on High Birefringence Fiber

Author(s):  
Manuel Durn-Snchez ◽  
R. Ivn ◽  
Evgeny A. ◽  
Baldemar Ibarra-Escamilla ◽  
Andrs Gonzlez-Garca ◽  
...  
Laser Physics ◽  
2009 ◽  
Vol 20 (2) ◽  
pp. 522-527 ◽  
Author(s):  
H. B. Sun ◽  
X. M. Liu ◽  
Y. K. Gong ◽  
X. H. Li ◽  
L. R. Wang

2018 ◽  
Vol 98 ◽  
pp. 56-60 ◽  
Author(s):  
Pan Fu ◽  
Xiao-qiang Feng ◽  
Baole Lu ◽  
Xin-yuan Qi ◽  
Haowei Chen ◽  
...  

2008 ◽  
Vol 6 (11) ◽  
pp. 818-820 ◽  
Author(s):  
许鸥 Ou Xu ◽  
鲁韶华 Shaohua Lu ◽  
冯素春 Suchun Feng ◽  
简水生 Shuisheng Jian

2011 ◽  
Vol 50 (3) ◽  
pp. 253 ◽  
Author(s):  
R. I. Álvarez-Tamayo ◽  
M. Durán-Sánchez ◽  
O. Pottiez ◽  
E. A. Kuzin ◽  
B. Ibarra-Escamilla ◽  
...  

2014 ◽  
Vol 4 (3) ◽  
pp. 225-229 ◽  
Author(s):  
Haifeng Qi ◽  
Zhiqiang Song ◽  
Jian Guo ◽  
Chang Wang ◽  
Jun Chang ◽  
...  

2011 ◽  
Vol 20 (04) ◽  
pp. 443-451
Author(s):  
M. R. A. MOGHADDAM ◽  
S. W. HARUN ◽  
S. SHAHI ◽  
H. AHMAD

A dual wavelength high power double-clad erbium/ytterbium-doped fiber laser with a narrowest spacing of 0.4 nm and a M2 value of close to unity is presented in the region of 1565 nm. This result can be realized with a significant improvement of the mode competition problem using a loop mirror as a comb filter. The wavelength region can also be varied using polarization controllers in the loop mirror. This dual-wavelength fiber laser with side mode suppression ratio (SMSR) of 40 dB is quite stable, and the output power variance is as low as 0.46 dB.


2021 ◽  
Author(s):  
Abdul Hadi Sulaiman ◽  
Nur Maizatul Nadia Najamhuri ◽  
Muhd Amirul Hafizi Sukor ◽  
Aiman Ismail ◽  
Fairuz Abdullah ◽  
...  

This paper demonstrates a multiwavelength fiber laser (MWFL) with erbiumdoped fiber amplifier (EDFA) as gain  medium and Sagnac loop mirror interferometer as filter. Stable and flat lasing spectrum was achieved when highly  nonlinear fiber (HNLF) was inserted into the laser cavity. The number of lasing lines and extinction ratio (ER) was directly influenced by EDFA gain where at maximum setting, 14 lasing lines with ER of 19 dB were generated. The  stable and flat spectrum achieved spanned about 1.6 nm. This is due to the induced intensity dependent loss  mechanism in the cavity by adjusting the half-wave plate of the polarization controller in combination with the  HNLF. The MWFL output showed peak power variation of about 2.1 dB within 100 minutes of observation time.


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