scholarly journals All-Chalcogenide Ring Fiber Laser

Author(s):  
Mohsen Rezaei ◽  
Martin Rochette

Abstract We demonstrate the first all-chalcogenide Brillouin fiber laser as well as the first all-chalcogenide ring cavity laser. The compact device comprises two engineered components: an As2Se3 optical fiber coupler combined to an As2S3 amplifying fiber. While the coupler simultaneously enables insertion of pump light, extraction of laser light, and the formation of a ring cavity, the amplifying fiber provides nonlinear gain to ensure laser oscillation. Thanks to the strong Brillouin gain of As2S3, only 3 m of amplifying fiber is required, thus making a resonant cavity with a free spectral range significantly larger than the Brillouin gain spectrum. The laser therefore naturally enables single longitudinal mode operation without additional filtering device. Acting as a coherence enhancing component, the resulting Brillouin laser benefits of a linewidth reduction factor of 7 with respect to the pump laser. Finally, this laser design is compatible with a broad range of wavelengths that spreads from 1.55 µm up to 8 µm, thanks to its all-chalcogenide structure.

2014 ◽  
Vol 1044-1045 ◽  
pp. 426-431
Author(s):  
Wu Pan ◽  
Hong Lin Zhang ◽  
Zheng Ke Xu ◽  
Hui Zhang

In order to realize single longitudinal mode (SLM) output, an erbium-doped fiber (EDF) laser with fiber ring cavity is proposed which uses an un-pumped EDF saturated absorber as a SLM selector. Ring cavity length, coupler ratio and insertion loss which affect ring cavity filter performance are analyzed theoretically and simulated numerically. Un-pumped EDF length and Er3+ concentration are analyzed theoretically and simulated. Research shows that, the bigger coupling output ratio of ring cavity, the greater transmission peak; the greater mode line width; the shorter ring cavity length, the wider free spectral range; the bigger coupling loss, the smaller transmission peak; when the difference between two cavities length is big, cursor effect is not obvious. Laser threshold increases with absorber length increasing; the bigger saturated absorber concentration, the higher laser threshold.


1998 ◽  
Author(s):  
Chien-Chung Lee ◽  
Yung Kung Chen ◽  
Shien-Kuei Liaw ◽  
Frank Tsai ◽  
Ching Sheu Wang ◽  
...  

2017 ◽  
Vol 9 (1) ◽  
pp. 1-7 ◽  
Author(s):  
Wencai Li ◽  
Haowei Liu ◽  
Ji Zhang ◽  
Bo Yao ◽  
Sujuan Feng ◽  
...  

2011 ◽  
Vol 23 (22) ◽  
pp. 1658-1660 ◽  
Author(s):  
Feifei Yin ◽  
Sigang Yang ◽  
Hongwei Chen ◽  
Minghua Chen ◽  
Shizhong Xie

2009 ◽  
Vol 36 (7) ◽  
pp. 1890-1893 ◽  
Author(s):  
俞力 Yu Li ◽  
宋跃江 Song Yuejiang ◽  
张旭苹 Zhang Xuping

2021 ◽  
Vol 48 (5) ◽  
pp. 0501017
Author(s):  
刘昊炜 Liu Haowei ◽  
张骥 Zhang Ji ◽  
魏珊珊 Wei Shanshan ◽  
姚波 Yao Bo ◽  
毛庆和 Mao Qinghe

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