• Matter and Radiation at Extremes
  • Vol. 10, Issue 2, 029901 (2025)
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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    DOI: 10.1063/5.0253622 Cite this Article
    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 Copy Citation Text show less
    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.
    Fig. 1. 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.”
    Fig. 2. 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.”
    Fig. 3. Corrected graph of Fig. 5: “Electron energy spectra measured at 13.5° by SESAME on shots #176, #177, and #178.”
    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 1. Corrected values of Table I: “Summary of hot-electron measurements using the SESAME diagnostics.”
    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
    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.”
    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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