• Matter and Radiation at Extremes
  • Vol. 4, Issue 6, 064403 (2019)
Yan-Jun Gu1、2、a), Martin Jirka1、3, Ondrej Klimo1、3, and Stefan Weber1、4
Author Affiliations
  • 1Institute of Physics of the ASCR, ELI-Beamlines, Na Slovance 2, 18221 Prague, Czech Republic
  • 2Institute of Plasma Physics of the CAS, Za Slovankou 1782/3, 18200 Prague, Czech Republic
  • 3FNSPE, Czech Technical University in Prague, 11519 Prague, Czech Republic
  • 4School of Science, Xi’an Jiaotong University, Xi’an 710049 China
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    DOI: 10.1063/1.5098978 Cite this Article
    Yan-Jun Gu, Martin Jirka, Ondrej Klimo, Stefan Weber. Gamma photons and electron-positron pairs from ultra-intense laser-matter interaction: A comparative study of proposed configurations[J]. Matter and Radiation at Extremes, 2019, 4(6): 064403 Copy Citation Text show less
    Simulation results for two colliding laser pulses. (a) Schematic setup of the two-pulse collision regime. (b) Energy spectra for γ photons and positrons in both long- and short-pulse cases. (c) and (d) Angular distributions of energy for γ photons and positrons generated in the short-pulse case. (e) and (f) Corresponding results for the long-pulse case.
    Fig. 1. Simulation results for two colliding laser pulses. (a) Schematic setup of the two-pulse collision regime. (b) Energy spectra for γ photons and positrons in both long- and short-pulse cases. (c) and (d) Angular distributions of energy for γ photons and positrons generated in the short-pulse case. (e) and (f) Corresponding results for the long-pulse case.
    Simulation results for a single laser pulse with a plasma mirror. (a) Schematic setup of the regime. (b) Energy spectra for γ photons and positrons in both long- and short-pulse cases. (c) and (d) Angular distributions of energy for γ photons and positrons generated in the short-pulse case. (e) and (f) Corresponding results for the long-pulse case.
    Fig. 2. Simulation results for a single laser pulse with a plasma mirror. (a) Schematic setup of the regime. (b) Energy spectra for γ photons and positrons in both long- and short-pulse cases. (c) and (d) Angular distributions of energy for γ photons and positrons generated in the short-pulse case. (e) and (f) Corresponding results for the long-pulse case.
    Setupaɛγ〉 (GeV)Nγ (m−1)ηγ (%)εe+ (GeV)Ne+ (nC μm−1)ηe+ (%)
    A: τ = 15fs0.0146.4 × 10188.440.240.090.01
    A: τ = 150 fs0.0121.1 × 102012.40.23.280.04
    B: τ = 15 fs0.021.36 × 1019210.231.40.2
    B: τ = 150 fs0.0110209.80.220.03
    Table 1. Main simulation results for all setups: 〈ɛγ〉 and εe+ are the average energies of the γ photons and positrons; Nγ and Ne+ are the numbers of γ photons and positrons produced in the simulation box; ηγ and ηe+ are the laser energy conversion efficiencies to γ photons and positrons.
    Yan-Jun Gu, Martin Jirka, Ondrej Klimo, Stefan Weber. Gamma photons and electron-positron pairs from ultra-intense laser-matter interaction: A comparative study of proposed configurations[J]. Matter and Radiation at Extremes, 2019, 4(6): 064403
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