• High Power Laser Science and Engineering
  • Vol. 7, Issue 3, 03000e40 (2019)
Bao Du1, Hong-Bo Cai1,2,3,†, Wen-Shuai Zhang1, Shi-Yang Zou1..., Jing Chen1,2,3 and Shao-Ping Zhu1,4,5,†|Show fewer author(s)
Author Affiliations
  • 1Institute of Applied Physics and Computational Mathematics, Beijing 100094, China
  • 2HEDPS, Center for Applied Physics and Technology, Peking University, Beijing 100871, China
  • 3IFSA Collaborative Innovation Center, Shanghai Jiao Tong University, Shanghai 200240, China
  • 4STPPL, Research Center of Laser Fusion, China Academy of Engineering Physics, Mianyang 621900, China
  • 5Graduate School, China Academy of Engineering Physics, Beijing 100088, China
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    DOI: 10.1017/hpl.2019.30 Cite this Article Set citation alerts
    Bao Du, Hong-Bo Cai, Wen-Shuai Zhang, Shi-Yang Zou, Jing Chen, Shao-Ping Zhu, "A demonstration of extracting the strength and wavelength of the magnetic field generated by the Weibel instability from proton radiography," High Power Laser Sci. Eng. 7, 03000e40 (2019) Copy Citation Text show less
    Schematic diagram of proton radiography of a two-dimensionally isotropic and stochastic magnetic field.
    Fig. 1. Schematic diagram of proton radiography of a two-dimensionally isotropic and stochastic magnetic field.
    (a) Transversal cross-section of the pre-set stochastic magnetic field tubes at $y=2~\text{mm}$. (b) Two-dimensional spectrum of the magnetic field by taking Fourier transforms of the field in (a), which shows an isotropic feature.
    Fig. 2. (a) Transversal cross-section of the pre-set stochastic magnetic field tubes at $y=2~\text{mm}$. (b) Two-dimensional spectrum of the magnetic field by taking Fourier transforms of the field in (a), which shows an isotropic feature.
    One-dimensional energy spectrum of the magnetic field $E_{B}(k)$. The red line corresponds to the energy spectrum obtained by taking Fourier transforms of the pre-set magnetic field in Figure 2(a), whereas the blue line corresponds to the energy spectrum extracted from proton radiography with Equation (22).
    Fig. 3. One-dimensional energy spectrum of the magnetic field $E_{B}(k)$. The red line corresponds to the energy spectrum obtained by taking Fourier transforms of the pre-set magnetic field in Figure 2(a), whereas the blue line corresponds to the energy spectrum extracted from proton radiography with Equation (22).
    (a) Proton density perturbation $\unicode[STIX]{x1D6FF}n/n_{0}$ on the detection plane when $L_{D}=5~\text{cm}$. (b) The extracted two-dimensional distribution of $u_{y}$. (c) One-dimensional distributions of $u_{y}$ at $y=2~\text{mm}$ from the extracted results and the pre-settings.
    Fig. 4. (a) Proton density perturbation $\unicode[STIX]{x1D6FF}n/n_{0}$ on the detection plane when $L_{D}=5~\text{cm}$. (b) The extracted two-dimensional distribution of $u_{y}$. (c) One-dimensional distributions of $u_{y}$ at $y=2~\text{mm}$ from the extracted results and the pre-settings.
    Bao Du, Hong-Bo Cai, Wen-Shuai Zhang, Shi-Yang Zou, Jing Chen, Shao-Ping Zhu, "A demonstration of extracting the strength and wavelength of the magnetic field generated by the Weibel instability from proton radiography," High Power Laser Sci. Eng. 7, 03000e40 (2019)
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