scholarly journals Au nanocages saturable absorber for 3-µm mid-infrared pulsed fiber laser with a wide wavelength tuning range

2019 ◽  
Vol 27 (21) ◽  
pp. 30350 ◽  
Author(s):  
Qingru Li ◽  
Chen Wei ◽  
Hao Chi ◽  
Liqiang Zhou ◽  
Han Zhang ◽  
...  
2017 ◽  
Vol 29 (11) ◽  
pp. 881-884 ◽  
Author(s):  
Chen Wei ◽  
Han Zhang ◽  
H. Shi ◽  
K. Konynenbelt ◽  
H. Luo ◽  
...  

AIP Advances ◽  
2018 ◽  
Vol 8 (2) ◽  
pp. 025121 ◽  
Author(s):  
Shougui Ning ◽  
Guoying Feng ◽  
Shenyu Dai ◽  
Hong Zhang ◽  
Wei Zhang ◽  
...  

2016 ◽  
Vol 13 (10) ◽  
pp. 105108 ◽  
Author(s):  
Chen Wei ◽  
Hongyu Luo ◽  
Han Zhang ◽  
Chun Li ◽  
Jitao Xie ◽  
...  

2020 ◽  
Vol 58 ◽  
pp. 102249
Author(s):  
M. Adzimnuddin ◽  
A.A. Latiff ◽  
H. Hazura ◽  
M.T. Ahmad ◽  
M.A. Azam ◽  
...  

2019 ◽  
Vol 1372 ◽  
pp. 012003
Author(s):  
Arni Munira Markom ◽  
Muhammad Taufiq Ahmad ◽  
Hazlihan Haris ◽  
Ahmad Razif Muhammad ◽  
Zakiah Mohd Yusoff ◽  
...  

1999 ◽  
Vol 607 ◽  
Author(s):  
H. Q. Le ◽  
C.-H. Lin ◽  
S. J. Murry ◽  
J. Zheng ◽  
S.-S. Pei

AbstractSb mid-IR laser can be used in external configuration to achieve wide wavelength tuning range. At low temperature, gain media with band-edge wavelengths between 3.3 to 4 pm have been demonstrated with wavelength tuning up to ∼9% of the center wavelength. Power output from few tens of mW to 0.2-W peak, 20-mW average was achieved. Type-II Sb laser promises the possibility of such performance at higher temperature, e. g. 200 K. However, significant trade-off must be considered between tuning range and power and efficiency. Optimization requires consideration of both basic wafer design and cavity geometry.


Author(s):  
Tao Zhang ◽  
Guoying Feng ◽  
Hong Zhang ◽  
Xianheng Yang ◽  
Bin Lan ◽  
...  

2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Yin-Wen Lee ◽  
Chien-Ming Chen ◽  
Wei-Hsiang Chuang ◽  
Ching-Yi Cho ◽  
Cheng-Hsien Yu ◽  
...  

AbstractMode-locked and Q-switched pulsed fiber laser sources with wavelengths of 1.55 μm are widely used in various fields. Gold nanorods (GNRs) have been applied in biomedicine and optics owing to their biocompatibility, easy fabrication, and unique optical properties. This paper presents the analysis of a saturable absorber based on a colloidal gold nanorod (GNR) thin film for dual-function passively mode-locked and Q-switched 1.55-μm fiber lasers. The colloidal GNR thin film possesses superior properties such as a wide operating wavelength range, large nonlinear absorption coefficient, and a picosecond-order recovery time. Its modulation depth and saturation intensity at 1.55 μm are 7.8% and 6.55 MW/cm2, respectively. Passive mode-locked or Q-switched laser operation is achieved by changing the number of GNR thin-film layers. The advantages of these high-quality GNRs in mode-locked and Q-switched fiber lasers with record-high slope efficiency are verified by conducting comprehensive material and laser dynamic analyses. The self-starting mode-locked fiber laser with an efficiency as high as 24.91% and passively Q-switched fiber laser with the maximum energy of 0.403 μJ are successfully demonstrated. This paper presents the novel demonstration of reconfigurable mode-locked and Q-switched all-fiber lasers by incorporating colloidal GNR thin films.


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