High Power Laser Science and Engineering, Volume. 6, Issue 3, 03000e38(2018)
Generation of strong magnetic fields with a laser-driven coil
Fig. 3. The number of escaping electrons per unit laser energy as a function of .
Fig. 4. Typical symmetric signal observed with a differential twisted pair[38].
Fig. 5. Example of a Faraday rotation measurement: (a) typical setup; (b) reference image; (c) image in the presence of a -field[32].
Fig. 6. Example of a proton deflectometry measurement: (a) schematic of the setup; (b) image obtained on RCF with 13 MeV protons; (c) simulation of proton deflection in a -field[35].
Fig. 7. Minimum electron energy required for electron deflectometry, as a function of the product .
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Zhe Zhang, Baojun Zhu, Yutong Li, Weiman Jiang, Dawei Yuan, Huigang Wei, Guiyun Liang, Feilu Wang, Gang Zhao, Jiayong Zhong, Bo Han, Neng Hua, Baoqiang Zhu, Jianqiang Zhu, Chen Wang, Zhiheng Fang, Jie Zhang. Generation of strong magnetic fields with a laser-driven coil[J]. High Power Laser Science and Engineering, 2018, 6(3): 03000e38
Special Issue: LABORATORY ASTROPHYSICS
Received: Nov. 28, 2017
Accepted: May. 9, 2018
Published Online: Aug. 28, 2018
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