scholarly journals Controlling the phase matching conditions of optical parametric chirped-pulse amplification using partially deuterated KDP

2009 ◽  
Vol 17 (10) ◽  
pp. 7744 ◽  
Author(s):  
K. Ogawa ◽  
K. Sueda ◽  
Y. Akahane ◽  
M. Aoyama ◽  
K. Tsuji ◽  
...  
2014 ◽  
Vol 330 ◽  
pp. 24-29 ◽  
Author(s):  
Xiaoyang Guo ◽  
Yi Xu ◽  
Xiao Zou ◽  
Xiaoming Lu ◽  
Yanyan Li ◽  
...  

2005 ◽  
Vol 246 (4-6) ◽  
pp. 323-330 ◽  
Author(s):  
Cheng Wang ◽  
Yuxin Leng ◽  
Xiaoyan Liang ◽  
Baozhen Zhao ◽  
Zhizhan Xu

2018 ◽  
Vol 167 ◽  
pp. 01006 ◽  
Author(s):  
Marco Galimberti ◽  
Alexis Boyle ◽  
Ian O. Musgrave ◽  
Pedro Oliveira ◽  
Dave Pepler ◽  
...  

The Optical Parametric Chirped Pulse Amplification is one of the most promising techniques to deliver 20PW laser system. The already available KD*P in large size is a good candidate as nonlinear crystal. In this article we report the experimental analysis of the spectral small signal gain for KD*P at 70% deuteration level for different phase matching and non-collinear angle. The data is also compared with a theoretical model.


2021 ◽  
Author(s):  
Ji Wang ◽  
Yanqing Zheng ◽  
Yunlin Chen

Abstract Optical parametric chirped pulse amplification (OPCPA) shows great potential in producing ultrashort high-intensity pulses because of its large gain bandwidth. Quasi-parametric chirped pulse amplification (QPCPA) may further extend the bandwidth, but the behavior of QPCPA at a limited pump intensity (e.g., ≤5 GW/cm2 in a nanosecond pumped QPCPA) is not fully investigated yet. We have discussed in detail the ultra-broadband amplification and the noncollinear phase-matching geometry in QPCPA. We have modeled and developed a novel noncollinear geometry in QPCPA namely ’triple-wavelength phase-matching geometry’ which provides two additional phase-matching points around the phase-matching point at the center wavelength. Our analysis demonstrates that the triple-wavelength phase-matching geometry can support stable, ultra-broadband amplification in QPCPA. The numerical simulation results show that ultrashort pulse with a pulse duration of 7.92 fs can be achieved in QPCPA when the pump intensity is limited to 5 GW/cm2, calculated using the nonlinear coefficient of YCOB.


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