A laser wakefield acceleration facility using SG-II petawatt laser system

Laser wakefield acceleration (LWFA) using PW-class laser pulses generally requires cm-scale laser–plasma interaction Rayleigh length, which can be realized by focusing such pulses inside a long underdense plasma with a large f-number focusing optic. Here, we present a new PW-based LWFA instrument at...

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Veröffentlicht in:Review of scientific instruments 2022-03, Vol.93 (3), p.033504-033504
Hauptverfasser: Liang, Xiao, Yi, Youjian, Li, Song, Zhu, Ping, Xie, Xinglong, Liu, Huiya, Mu, GuangJin, Liu, ZhiGang, Guo, Ailin, Kang, Jun, Yang, Qingwei, Zhu, Haidong, Gao, Qi, Sun, Meizhi, Lu, Haiyang, Ma, Yanyun, Mondal, Sudipta, Papp, Dániel, Majorosi, Szilárd, Lécz, Zsolt, Andreev, Alexander, Kahaly, Subhendu, Kamperidis, Christos, Hafz, Nasr A. M., Zhu, Jianqiang
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Sprache:eng
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Zusammenfassung:Laser wakefield acceleration (LWFA) using PW-class laser pulses generally requires cm-scale laser–plasma interaction Rayleigh length, which can be realized by focusing such pulses inside a long underdense plasma with a large f-number focusing optic. Here, we present a new PW-based LWFA instrument at the SG-II 5 PW laser facility, which employs f/23 focusing. The setup also adapted an online probing of the plasma density via Nomarski interferometry using a probe laser beam having 30 fs pulse duration. By focusing 1-PW, 30-fs laser pulses down to a focal spot of 230 µm, the peak laser intensity reached a mild-relativistic level of 2.6 × 1018 W/cm2, a level modest for standard LWFA experiments. Despite the large aspect ratio of >25:1 (transverse to longitudinal dimensions) of the laser pulse, electron beams were observed in our experiment only when the laser pulse experienced relativistic self-focusing at high gas-pressure thresholds, corresponding to plasma densities higher than 3 × 1018 cm−3.
ISSN:0034-6748
1089-7623
DOI:10.1063/5.0071761