Matter and Radiation at Extremes, Volume. 9, Issue 2, 027201(2024)

Characterization of bright betatron radiation generated by direct laser acceleration of electrons in plasma of near critical density

J. Cikhardt1、a), M. Gyrdymov2, S. Zähter3,4, P. Tavana2, M. M. Günther3, N. Bukharskii5,6, N. Borisenko6, J. Jacoby2, X. F. Shen7, A. Pukhov7, N. E. Andreev8,9, and O. N. Rosmej2,3
Author Affiliations
  • 1Faculty of Electrical Engineering, Czech Technical University in Prague, 16627 Prague 6, Czech Republic
  • 2Goethe University, Frankfurt, Max-von-Laue-Straße 1, 60438 Frankfurt am Main, Germany
  • 3GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, 64291 Darmstadt, Germany
  • 4Focused Energy GmbH, Im Tiefen See 45, 64293 Darmstadt, Germany
  • 5National Research Nuclear University MEPhI, Kashirskoe shosse 31, 115409 Moscow, Russian Federation
  • 6Lebedev Physical Institute RAS, Leninskiy Prospekt 53, 119991 Moscow, Russian Federation
  • 7Heinrich-Heine-University Düsseldorf, Universitätsstrasse 1, Düsseldorf, Germany
  • 8Joint Institute for High Temperatures, RAS, Izhorskaya st. 13, Bldg. 2, 125412 Moscow, Russian Federation
  • 9Moscow Institute of Physics and Technology, Institutskiy Pereulok 9, 141700 Dolgoprudny, Russia
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    Figures & Tables(19)
    Schematic of experimental arrangement.
    X-ray detector. (a) 3D model of detector. (b) Photograph of prepared detector with a set of Ross filters. (c) Example of image plate signal, where the individual filters are labeled by the foil material and thickness in micrometers.
    Photon transmission characteristics of thin filters.
    Differential photon transmission characteristics of thin filter pairs.
    Photon transmission characteristics of thick filters.
    Differential photon transmission characteristics of thick filter pairs.
    Examples of semiconductor diode signal: (a) without proton/ion shielding; (b) with proton shielding by 560 μm thick Mylar foil.
    Example of outputs from individual channels of the Ross filter spectrometer in shots with and without proton/ion shielding.
    Electron spectra from shots without (red and green) and with (blue) the deflection magnetic field.
    Deflection of electrons by the magnetic yoke as a function of electron energy.
    Examples of IP signals behind the set of thin filters from the shot with 580 μm foam target and 66 J in the main pulse.
    Betatron radiation spectrum from a shot with a 580 μm thick foam target in the directions of 0° and 10°.
    Spectrum of betatron radiation in the directions of 0° and 10° evaluated with a help of thick filters.
    X-ray spectra for different 2 mg/cm3 foam thicknesses evaluated with the help of the thin filters set placed at 0° to the laser axis.
    X-ray spectra from shots evaluated with the help of the thick filters placed at 0° to the laser axis.
    Comparison of betatron radiation spectra from the experiments using thin filters (66 J, 580 μm foam) and thick filters (76 J, 470 μm) with the 3D-PIC simulation.
    • Table 1. Dependence of x-ray (≥15 keV) signal amplitude on foam thickness for 1013 W/cm2, 3 ns pulse and 1019 W/cm2 main pulse with 3 ns delay. The x-ray diode shielding is 12.5 μm Ti and two IPs.

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      Table 1. Dependence of x-ray (≥15 keV) signal amplitude on foam thickness for 1013 W/cm2, 3 ns pulse and 1019 W/cm2 main pulse with 3 ns delay. The x-ray diode shielding is 12.5 μm Ti and two IPs.

      ShotTargetps-pulse energy (J)X-ray pulse (V)
      No. 36Foam, 460 µm71∼9
      No. 42Foam, 800 µm7016
      No. 44Foam, 1000 µm757
      No. 43Foam, 1500 µm703
    • Table 2. Dependence of the x-ray (≥15 keV) signal amplitude on ns-pulse intensity: from 1013 W/cm2 up to ∼1014 W/cm2 (duration 3 ns, delay 3 ns). The x-ray diode shielding is 12.5 μm Ti and two IPs.

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      Table 2. Dependence of the x-ray (≥15 keV) signal amplitude on ns-pulse intensity: from 1013 W/cm2 up to ∼1014 W/cm2 (duration 3 ns, delay 3 ns). The x-ray diode shielding is 12.5 μm Ti and two IPs.

      ShotTargetns-pulse intensity (W/cm2)ps-pulse energy (J)X-ray pulse (V)
      No. 36Foam, 460 µm101371∼9
      No. 47Foam, 400 µm10147829
      No. 44Foam, 1000 µm1013757
      No. 46Foam, 1000 µm10148019
    • Table 3. Dependence of x-ray (≥15 keV) signal amplitude on target material.

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      Table 3. Dependence of x-ray (≥15 keV) signal amplitude on target material.

      ShotTargetns-pulse intensity (W/cm2)ps-pulse energy (J)X-ray pulse (V)
      No. 47Foam, 400 µm10147829
      No. 46Foam, 1000 µm3 × 10138019
      No. 54Mylar, 0.9 µmNo ns pulse701.3
      No. 56Gold, 0.96 µmNo ns pulse765
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    J. Cikhardt, M. Gyrdymov, S. Zähter, P. Tavana, M. M. Günther, N. Bukharskii, N. Borisenko, J. Jacoby, X. F. Shen, A. Pukhov, N. E. Andreev, O. N. Rosmej. Characterization of bright betatron radiation generated by direct laser acceleration of electrons in plasma of near critical density[J]. Matter and Radiation at Extremes, 2024, 9(2): 027201

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    Paper Information

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    Received: Oct. 14, 2023

    Accepted: Jan. 16, 2024

    Published Online: Apr. 15, 2024

    The Author Email: Cikhardt J. (cikhajak@fel.cvut.cz)

    DOI:10.1063/5.0181119

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