Highly reliable, high-brightness 915nm laser diodes for fiber laser applications

Author(s):  
Zuntu Xu ◽  
Wei Gao ◽  
Lisen Cheng ◽  
Kejian Luo ◽  
Kun Shen ◽  
...  
2014 ◽  
Author(s):  
D. M. Hemenway ◽  
Wolfram Urbanek ◽  
Kylan Hoener ◽  
Keith W. Kennedy ◽  
Ling Bao ◽  
...  

Sensors ◽  
2021 ◽  
Vol 21 (1) ◽  
pp. 239
Author(s):  
Lingling Yang ◽  
Ruwei Zhao ◽  
Duanduan Wu ◽  
Tianxiang Xu ◽  
Xiaobiao Liu ◽  
...  

A novel 2H-phase transition metal dichalcogenide (TMD)–tantalum selenide (TaSe2) with metallic bandgap structure is a potential photoelectric material. A band structure simulation of TaSe2 via ab initio method indicated its metallic property. An effective multilayered TaSe2 saturable absorber (SA) was fabricated using liquid-phase exfoliation and optically driven deposition. The prepared 2H–TaSe2 SA was successfully used for a dual-wavelength Q-switched fiber laser with the minimum pulse width of 2.95 μs and the maximum peak power of 64 W. The repetition rate of the maximum pulse energy of 89.9 kHz was at the level of 188.9 nJ. The metallic 2H–TaSe2 with satisfactory saturable absorbing capability is a promising candidate for pulsed laser applications.


2021 ◽  
Vol 48 (5) ◽  
pp. 0501016
Author(s):  
丁兵 Ding Bing ◽  
赵鹏飞 Zhao Pengfei ◽  
段程芮 Duan Chengrui ◽  
娄博杰 Lou Bojie ◽  
林学春 Lin Xuechun

2009 ◽  
Vol 35 (4) ◽  
pp. 189-198
Author(s):  
Yousuke KAWAHITO ◽  
Masami MIZUTANI ◽  
Seiji KATAYAMA

2011 ◽  
Vol 38 (8) ◽  
pp. 0801001
Author(s):  
许晓军 Xu Xiaojun ◽  
杨子宁 Yang Zining ◽  
王红岩 Wang Hongyan ◽  
陆启生 Lu Qisheng

2011 ◽  
Vol 32 (10) ◽  
pp. 1064-1068
Author(s):  
YANG Ye ◽  
LIU Yun ◽  
ZHANG Jin-long ◽  
LI Zai-jin ◽  
SHAN Xiao-nan ◽  
...  

Author(s):  
Zehui Wang ◽  
Qirong Xiao ◽  
Yusheng Huang ◽  
Jiading Tian ◽  
Dan Li ◽  
...  

In this paper, we reported both the experimental demonstration and theoretical analysis of a Raman fiber laser based on a master oscillator–power amplifier configuration. The Raman fiber laser adopted the dual-wavelength bidirectional pumping configuration, utilizing 976 nm laser diodes and 1018 nm fiber lasers as the pump sources. A 60-m-long $25/400~\unicode[STIX]{x03BC}\text{m}$ ytterbium-doped fiber was used to convert the power from 1070 to 1124 nm, realizing a maximum power output of 3.7 kW with a 3 dB spectral width of 6.8 nm. Moreover, we developed a multi-frequency model taking into consideration the Raman gain spectrum and amplified spontaneous emission. The calculated spectral broadening of both the forward and backward laser was in good agreement with the experimental results. Finally, a 1.5 kW, 1183 nm second-order Raman fiber laser was further experimentally demonstrated by the addition of a 70-m-long germanium-doped passive fiber.


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