Efficient diode-pumped yellow, orange and red laser sources based on stimulated Raman scattering in KGd (WO4)2

2004 ◽  
Author(s):  
R.P. Mildren ◽  
H.M. Pask ◽  
M. Convery ◽  
J.A. Piper ◽  
T. Mckay
Keyword(s):  
Raman Scattering ◽  
Stimulated Raman Scattering ◽  
Yellow Orange ◽  
Diode Pumped ◽  
Laser Sources ◽  
Stimulated Raman

Progress and Prospects of Fiber Gas Laser Sources (Ⅰ) :Based on Stimulated Raman Scattering

2021 ◽  
Vol 48 (4) ◽  
pp. 0401008
Author(s):  
王泽锋 Wang Zefeng ◽  
黄威 Huang Wei ◽  
李智贤 Li Zhixian ◽  
周智越 Zhou Zhiyue ◽  
崔宇龙 Cui Yulong ◽  
...  
Keyword(s):  
Raman Scattering ◽  
Stimulated Raman Scattering ◽  
Gas Laser ◽  
Laser Sources ◽  
Stimulated Raman

scholarly journals Mitigation of stimulated Raman scattering in kilowatt-level diode-pumped fiber amplifiers with chirped and tilted fiber Bragg gratings

2019 ◽  
Vol 7 ◽  
Author(s):  
Meng Wang ◽  
Le Liu ◽  
Zefeng Wang ◽  
Xiaoming Xi ◽  
Xiaojun Xu
Keyword(s):  
Raman Scattering ◽  
Fiber Lasers ◽  
Stimulated Raman Scattering ◽  
Beam Quality ◽  
Average Power ◽  
Fiber Amplifiers ◽  
Maximum Output ◽  
Power Scaling ◽  
Diode Pumped ◽  
Stimulated Raman

The average power of diode-pumped fiber lasers has been developed deeply into the kW regime in the past years. However, stimulated Raman scattering (SRS) is still a major factor limiting the further power scaling. Here, we have demonstrated the mitigation of SRS in kilowatt-level diode-pumped fiber amplifiers using a chirped and tilted fiber Bragg grating (CTFBG) for the first time. The CTFBG is designed and inscribed in large-mode-area (LMA) fibers, matching with the operating wavelength of the fiber amplifier. With the CTFBG inserted between the seed laser and the amplifier stage, an SRS suppression ratio of ${\sim}10~\text{dB}$ is achieved in spectrum at the maximum output laser power of 2.35 kW, and there is no reduction in laser slope efficiency and degradation in beam quality. This work proves the feasibility and practicability of CTFBGs for SRS suppression in high-power fiber lasers, which is very useful for the further power scaling.

Stimulated Raman Scattering in YVO4 and GdVO4 Crystals and Self Raman Frequency Conversion in Diode Pumped Nd3+:GdVO4 Laser

2004 ◽  
Author(s):  
Tasoltan T. Basiev ◽  
Peter G. Zverev ◽  
Alexander Ya. Karasik ◽  
Sergey V. Vassiliev ◽  
Alexander A. Sobol ◽  
...  
Keyword(s):  
Raman Scattering ◽  
Frequency Conversion ◽  
Stimulated Raman Scattering ◽  
Raman Frequency ◽  
Diode Pumped ◽  
Stimulated Raman

Efficient self-stimulated Raman scattering with simultaneously self-mode-locking in a diode-pumped Nd:GdVO_4 laser

2016 ◽  
Vol 55 (32) ◽  
pp. 9000 ◽  
Author(s):  
Zuohan Li ◽  
Jiying Peng ◽  
Jianquan Yao ◽  
Ming Han ◽  
Linghong Jiang
Keyword(s):  
Raman Scattering ◽  
Stimulated Raman Scattering ◽  
Mode Locking ◽  
Diode Pumped ◽  
Stimulated Raman

Closed-Form Calculation of Coherent Anti-Stokes Raman and Stimulated Raman Scattering Spectral Profiles

1981 ◽  
Vol 35 (3) ◽  
pp. 276-278 ◽  
Author(s):  
P. E. Perkins ◽  
J. W. L. Lewis
Keyword(s):  
Raman Scattering ◽  
Closed Form ◽  
Stimulated Raman Scattering ◽  
Third Order ◽  
The Third ◽  
Spectral Profiles ◽  
Laser Sources ◽  
Anti Stokes ◽  
Order Susceptibility ◽  
Stimulated Raman

The third-order susceptibility is expressed as a summation of interfering resonant terms, each involving the phenomenological linewidth of the transition. Correlations of the finite linewidth of the laser sources with |χ(3)|2 (coherent anti-Stokes Raman spectroscopy) and –χ” (stimulated Raman scattering) are performed and closed-form expressions for the theoretical profiles are obtained.

scholarly journals Real-time Stimulated Raman Scattering Microscopy Using Fiber-laser Sources

2013 ◽  
Vol 41 (8) ◽  
pp. 619
Author(s):  
Yasuyuki OZEKI ◽  
Tatsuya KISHI ◽  
Keisuke NOSE ◽  
Kazuyoshi ITOH
Keyword(s):  
Raman Scattering ◽  
Fiber Laser ◽  
Real Time ◽  
Stimulated Raman Scattering ◽  
Laser Sources ◽  
Stimulated Raman
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