Matter and Radiation at Extremes, Volume. 10, Issue 2, 029901(2025)

Erratum: “Enhanced ion acceleration using the high-energy petawatt PETAL laser” [Matter Radiat. Extremes 6, 056901 (2021)]

D. Raffestin1...2,a), L. Lecherbourg3, I. Lantuéjoul3, B. Vauzour3, P. E. Masson-Laborde3,4, X. Davoine3,4, N. Blanchot1, J. L. Dubois1,2, X. Vaisseau3, E. d’Humières2, L. Gremillet3,4, A. Duval3, Ch. Reverdin3, B. Rosse3, G. Boutoux3, J. E. Ducret5, Ch. Rousseaux3, V. Tikhonchuk2,6 and D. Batani2 |Show fewer author(s)
Author Affiliations
  • 1CEA, DAM, CESTA, F-33116 Le Barp, France
  • 2Centre Laser Intenses et Applications, Université de Bordeaux–CNRS–CEA, UMR 5107, 33405 Talence, France
  • 3CEA, DAM, DIF, F-91297 Arpajon, France
  • 4Université Paris–Saclay, CEA, LMCE, 91680 Bruyères-le-Châtel, France
  • 5CEA, DRF, IRFU, GANIL, F-14000 Caen, France
  • 6ELI-Beamlines Research Centre, 25241 Dolní Břežany, Czech Republic
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    Figures & Tables(5)
    Schematic of the SESAME magnetic spectrometer. Negative charge particle (e−) trajectories are represented in red, positive charge particle (e+, p+) trajectories are represented in blue and neutral charge particle (n, γ) trajectories are represented in green.
    Corrected graph of Fig. 4: “Electron energy spectra measured at 13.5° and 58.5° from the rear target normal by SESAME on shot #176.”
    Corrected graph of Fig. 5: “Electron energy spectra measured at 13.5° by SESAME on shots #176, #177, and #178.”
    • Table 1. Corrected values of Table I: “Summary of hot-electron measurements using the SESAME diagnostics.”

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      Table 1. Corrected values of Table I: “Summary of hot-electron measurements using the SESAME diagnostics.”

      Shot #Hot electron temperature (MeV)Number of electrons above 2.5 MeV
      1764.902.4 · 1012
      1773.291.0 · 1012
      1781.793.0 · 1011
    • Table 2. Corrected values of Table II: “Estimation of ejected hot-electron charge using Eq. (1) and the value of the hot-electron velocity corresponding to the electron temperature obtained from the electron spectra shown in Fig. 5.”

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      Table 2. Corrected values of Table II: “Estimation of ejected hot-electron charge using Eq. (1) and the value of the hot-electron velocity corresponding to the electron temperature obtained from the electron spectra shown in Fig. 5.”

      Averaged microwave emissionTypical electron energy beforeTotal ejectedTotal number
      Shot #from 3 to 6 GHz (J/Hz)before deceleration (MeV)charge (μC)of ejected electrons
      1762 · 10−114.901.81.1 · 1013
      1772.2 · 10−113.2921.3 · 1013
      1785.7 · 10−121.791.27.7 · 1012
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    D. Raffestin, L. Lecherbourg, I. Lantuéjoul, B. Vauzour, P. E. Masson-Laborde, X. Davoine, N. Blanchot, J. L. Dubois, X. Vaisseau, E. d’Humières, L. Gremillet, A. Duval, Ch. Reverdin, B. Rosse, G. Boutoux, J. E. Ducret, Ch. Rousseaux, V. Tikhonchuk, D. Batani. Erratum: “Enhanced ion acceleration using the high-energy petawatt PETAL laser” [Matter Radiat. Extremes 6, 056901 (2021)][J]. Matter and Radiation at Extremes, 2025, 10(2): 029901

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    Paper Information

    Received: Dec. 18, 2024

    Accepted: Jan. 12, 2025

    Published Online: Apr. 30, 2025

    The Author Email: Raffestin D. (didier.raffestin@u-bordeaux.fr)

    DOI:10.1063/5.0253622

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