High peak power femtosecond cylindrical vector beams generation in a chirped-pulse amplification laser system

2022 ◽  
Vol 20 (3) ◽  
pp. 031405
Author(s):  
Zexing Zhao ◽  
Hao Chen ◽  
Ziming Zhang ◽  
Jiatong Li ◽  
Fangxiang Zhu ◽  
...  
Keyword(s):  
Peak Power ◽  
Laser System ◽  
High Peak ◽  
High Peak Power ◽  
Chirped Pulse ◽  
Pulse Amplification ◽  
Vector Beams ◽  
Chirped Pulse Amplification

scholarly journals Quasi-Parametric Chirped-Pulse Amplification Simultaneously Enables High Peak Power and High Average Power

2019 ◽  
Vol 11 (4) ◽  
pp. 1-12 ◽  
Author(s):  
Zhe Yin ◽  
Jingui Ma ◽  
Jing Wang ◽  
Peng Yuan ◽  
Guoqiang Xie ◽  
...  
Keyword(s):  
Peak Power ◽  
Average Power ◽  
High Peak ◽  
High Peak Power ◽  
High Average Power ◽  
Chirped Pulse ◽  
Pulse Amplification ◽  
Chirped Pulse Amplification

Hybrid vacuum-atmosphere compressors for ultrafast, high-peak power chirped-pulse amplification

1998 ◽  
Vol 4 (2) ◽  
pp. 441-444 ◽  
Author(s):  
B.C. Walker ◽  
J.A. Squier ◽  
D.N. Fittinghoff ◽  
C. Rose-Petruck ◽  
C.P.J. Barty
Keyword(s):  
Peak Power ◽  
High Peak ◽  
High Peak Power ◽  
Chirped Pulse ◽  
Pulse Amplification ◽  
Vacuum Atmosphere ◽  
Chirped Pulse Amplification

scholarly journals High-repetition-rate, high-peak-power 1450 nm laser source based on optical parametric chirped pulse amplification

2019 ◽  
Vol 7 ◽  
Author(s):  
Pengfei Wang ◽  
Beijie Shao ◽  
Hongpeng Su ◽  
Xinlin Lv ◽  
Yanyan Li ◽  
...  
Keyword(s):  
Repetition Rate ◽  
Peak Power ◽  
High Energy ◽  
High Peak ◽  
Laser Source ◽  
High Peak Power ◽  
Chirped Pulse ◽  
Pulse Amplification ◽  
Optical Parametric ◽  
Chirped Pulse Amplification

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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