scholarly journals Multi-Stage Optimization of Ultrabroadband High-Energy Optical Parametric Chirped Pulse Amplification

Author(s):  
Jeffrey Moses ◽  
Cristian Manzoni ◽  
Shu-Wei Huang ◽  
Giulio Cerullo ◽  
Franz X. Kärtner
2013 ◽  
Vol 38 (22) ◽  
pp. 4837 ◽  
Author(s):  
Lu Xu ◽  
Lianghong Yu ◽  
Xiaoyan Liang ◽  
Yuxi Chu ◽  
Zhanggui Hu ◽  
...  

2007 ◽  
Vol 32 (16) ◽  
pp. 2315 ◽  
Author(s):  
Hiromitsu Kiriyama ◽  
Michiaki Mori ◽  
Yoshiki Nakai ◽  
Yoichi Yamamoto ◽  
Manabu Tanoue ◽  
...  

2018 ◽  
Vol 20 (4) ◽  
pp. 224-231
Author(s):  
I.A. Kulagin ◽  
V.V. Gorbushin ◽  
B.R. Sobirov ◽  
V.V. Kim ◽  
T. Usmanov

Significant oscillations of the spectral distribution of the idler pulses in the optical parametric amplification of chirped laser pulse have been observed experimentally. On the base of the obtained simple analytical solution we have showed that such oscillations and an asymmetry of the spectral and temporal distributions of the intensities of the signal and the idler were caused by small variations in the parameters of the initial idler in comparison with the signal one. Conditions for distortion of the shape of the temporal and spectral distributions of the amplified compressed output pulses in a multi-stage laser with optical parametric chirped pulse amplification have been determined.


2015 ◽  
Vol 40 (14) ◽  
pp. 3412 ◽  
Author(s):  
Lianghong Yu ◽  
Xiaoyan Liang ◽  
Lu Xu ◽  
Wenqi Li ◽  
Chun Peng ◽  
...  

2008 ◽  
Vol 33 (20) ◽  
pp. 2386 ◽  
Author(s):  
Y. Tang ◽  
I. N. Ross ◽  
C. Hernandez-Gomez ◽  
G. H. C. New ◽  
I. Musgrave ◽  
...  

Author(s):  
Pengfei Wang ◽  
Beijie Shao ◽  
Hongpeng Su ◽  
Xinlin Lv ◽  
Yanyan Li ◽  
...  

We present a high-peak-power, near-infrared laser system based on optical parametric chirped pulse amplification pumped by a home-built picosecond pumping laser, which can generate over 40 mJ energy at 1450 nm center wavelength and operate at 100 Hz repetition rate. Subsequently, the chirped laser pulses are compressed down to 60 fs with 26.5 mJ energy, corresponding to a peak power of 0.44 TW. This high-energy, long-wavelength laser source is highly suitable for driving various nonlinear optical phenomena, such as high-order harmonic generation and high-flux coherent extreme ultraviolet/soft X-ray radiation.


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