scholarly journals Multi-Watt, mJ nanosecond pulses amplification in a Yb:LuLiF4 single crystal fiber grown by micro-pulling-down

2020 ◽  
Vol 243 ◽  
pp. 05001
Author(s):  
S. Pizzurro ◽  
F. Pirzio ◽  
S. Jun ◽  
A. Di Lieto ◽  
M. Tonelli ◽  
...  
Author(s):  
Igor Martial ◽  
François Balembois ◽  
Julien Didierjean ◽  
Patrick Georges

2021 ◽  
pp. 127337
Author(s):  
Sara Pizzurro ◽  
Federico Pirzio ◽  
Shu Jun ◽  
Alberto Di Lieto ◽  
Giuliano Piccinno ◽  
...  

2015 ◽  
Author(s):  
Xavier Délen ◽  
Adrien Aubourg ◽  
Loïc Deyra ◽  
Fabien Lesparre ◽  
Igor Martial ◽  
...  

2014 ◽  
Vol 37 ◽  
pp. 51-54 ◽  
Author(s):  
M.S. Silva ◽  
L.M. Jesus ◽  
L.B. Barbosa ◽  
D.R. Ardila ◽  
J.P. Andreeta ◽  
...  

2022 ◽  
Vol 43 (01) ◽  
pp. 42-50
Author(s):  
Xiao-fei MA ◽  
◽  
Tao WANG ◽  
Jian ZHANG ◽  
Yan-ru YIN ◽  
...  

2022 ◽  
Vol 148 ◽  
pp. 107744
Author(s):  
Sara Pizzurro ◽  
Shu Jun ◽  
Mauro Tonelli ◽  
Luca Carrá ◽  
Giuliano Piccinno ◽  
...  

Crystals ◽  
2019 ◽  
Vol 9 (4) ◽  
pp. 216
Author(s):  
Feng Li ◽  
Zhi Yang ◽  
Zhiguo Lv ◽  
Yang Yang ◽  
Yishan Wang ◽  
...  

A laser master oscillator power amplifier (MOPA) system consisting of a fiber amplifier and a two-stage Yb:YAG single crystal fiber (SCF) is experimentally studied. The nonlinear stimulated Raman scattering (SRS) is avoided by limiting the output power of the fiber preamplifier to 600 mW. Due to the benefit from the low nonlinearity and high amplification gain of the SCF, a laser pulse duration of 16.95 ps and a high average power of 41.7 W at a repetition rate of 250 kHz are obtained by using a two-stage polarization controlled double-pass amplification of Yb:YAG SCF, corresponding to an output energy of 166.8 μJ and a peak power of 9.84 MW, respectively. The polarization controlled SCF amplification scheme achieved a gain as high as more than 69 times. During the amplification, the spectra gain narrowing effect and the polarization controlled four-pass amplification setup are also studied. The laser spectrum is narrowed from over 10 nm to less than 3 nm, and the pulse width is also compressed to hundreds of femtosecond by dechirping the laser pulse. This compact-sized, cost-effective laser source can be used in laser micromachining, or as the seeder source for generating much higher power and energy laser for scientific research. For some applications which need femtosecond laser, this laser source can also be compressed to femtosecond regime.


Sign in / Sign up

Export Citation Format

Share Document