Matter and Radiation at Extremes, Volume. 6, Issue 1, 015401(2021)

The L4n laser beamline of the P3-installation: Towards high-repetition rate high-energy density physics at ELI-Beamlines

N. Jourdain1... U. Chaulagain1, M. Havlík1, D. Kramer1, D. Kumar1, I. Majerová1, V. T. Tikhonchuk1,2, G. Korn1, and S. Weber13,a) |Show fewer author(s)
Author Affiliations
  • 1ELI-Beamlines, Institute of Physics, Czech Academy of Sciences, 18221 Prague, Czech Republic
  • 2Centre Lasers Intenses et Applications, University of Bordeaux–CNRS–CEA, 33405 Talence, France
  • 3School of Science, Xi’an Jiaotong University, Xi’an 710049, China
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    Figures & Tables(13)
    The E3 experimental hall for plasma physics and beam configurations. The L4n pulse (1.9 kJ, 0.5 ns–10 ns, 1053 nm) is shown in pink. Three other beams will also be available in E3: L4f (1.5 kJ, 150 fs, 1053 nm), L4p (available in 2022) (150 J–400 J, 150 fs to 150 ps, 1053 nm), and L3 (30 J, 30 fs, 800 nm, 10 Hz).
    Schematic of the L4 ATON laser in the high-power non-CPA configuration.
    Layout of the compressor imaging system (CIS) with its optical scheme in the chirped pulse beamline (a) and with the M4.5 mirror position defined from Zemax OpticStudio simulations (b).
    (a) Design of the L4n beamline in the E3 experimental hall. The L4n beam is shown in pink up to the frequency-doubling KDP crystal. The converted 2ω beam is then shown in green. (b) Optical layout extracted from Zemax OpticStudio simulations.
    (a) Diffraction-limited focal spot with 0.2° lens tilt and 1 W input power in a square beam. (b) Focal spot with 0.42° lens tilt and 1 W input power in a square beam.
    Calculated KDP crystal conversion efficiency to second harmonic with 1 kJ as energy input.
    (a) Focal spot intensity profile (arbitrary units) simulated using wave front data from one of the phase plates. (b) Horizontal slice of the intensity profile.
    The left panels show laser pulse temporal profiles providing access to the Hugoniot adiabat and far-from-Hugoniot states. The right panels show the corresponding trajectories in the phase plane P–ρ. (a) Steady and quasi-isentropic compression. (b) Decaying shock and ramp compression. (c) Double shock. Adapted from Refs. 39,40.
    Configurations for multibeam experiments with L4n (green) and L3 (yellow) pulses: (a) long-focal-length (5 m) configuration in which L3 is focused in a gas jet and generates relativistic electrons and broadband hard X-rays at an angle of 112° with respect to the L4n beam; (b) short-focal-length (f = 750 mm) configuration in which the L3 pulse is focused by an off-axis parabola (OAP) at an angle of 58° with respect to the L4n beam.
    • Table 1. Overview of the current performance of major high-energy laser facilities in a long-pulse configuration listing the name of the installation, the operating entity, the laser wavelength in nanometers, the maximum energy available per shot, and the operating repetition rate.7

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      Table 1. Overview of the current performance of major high-energy laser facilities in a long-pulse configuration listing the name of the installation, the operating entity, the laser wavelength in nanometers, the maximum energy available per shot, and the operating repetition rate.7

      InstallationOperating facilityλ (nm)Maximum energy (long pulse)Repetition rate
      NIFLLNL (Livermore, USA)10532.1 MJ (3ω, 3 ns–15 ns)Every 8 h
      LMJCEA (Le Barp, France)10531.4 MJ (3ω, 3 ns–15 ns)Every 8 h
      Omega EPLLE (Rochester, USA)105330 kJ (3ω, 1 ns–3 ns)Every 90 min
      SG-II-UPSIOM (Shanghai, China)105324 kJ (3ω, 3 ns)Every 3 h
      Gekko XIIILE (Osaka, Japan)106410 kJ (2ω, 1 ns)Every 30 min
      OrionAWE (Aldermaston, UK)10535 kJ (3ω, 1 ns)Every 45 min
      L4nELI-Beamlines (Prague, Czech Republic)10531.2 kJ (2ω, 1 ns–5 ns)1 shot/min
      VULCANCLF, STFC (Oxford, UK)10531 kJ (2ω, 1 ns–10 ns)2 shots/day
      PALSIoP (Prague, Czech Republic)1315200 J (3ω, 250 ps)Every 25 min
      LULI 2000LULI, CEA (Paris, France)1053750 J (2ω, 1.5 ns)Every 90 min
      MECSLAC (Menlo Park, USA)105360 J (2ω, 10 ns)Every 7 min
      HIBEFEu-XFEL (Schenefeld, Germany)1053100 J (1ω, 10 ns)10 Hz
    • Table 2. L4n laser specifications.

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      Table 2. L4n laser specifications.

      Beam dimensions32 × 32 cm2
      Central wavelengthλ = 1053.2 nm
      Energy1.9 kJ
      Pulse durationτ = 0.1 ns–10 ns
      Strehl ratio∼0.5
      Pointing stability<10 µrad
      Beam shapeSquare super-Gaussian (order ∼20)
    • Table 3. Requirements on the nominal L4n design.

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      Table 3. Requirements on the nominal L4n design.

      RequirementSpecification
      Maximum energy 1ω1.9 kJ
      Maximum energy 2ω1 kJ
      Beam dimensions initial phase25 cm diameter
      Maximum energy 1ω subaperture beam1 kJ
      Conversion efficiencyBest effort >60%
      Best spot diameter50 µm
      Spot diameter after conditioning>300 µm
      Nominal focus position±2 mm lateral/±5 mm longitudinal
      Synchronization20 ps
      Pointing stability<5 µrad on KDP crystal
      Maximum repetition rate at 2ω1 shot/min
    • Table 4. Main specifications of frequency-doubling KDP crystal.

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      Table 4. Main specifications of frequency-doubling KDP crystal.

      Clear aperture284 ± 1 mm
      Phase matching angle59 ± 0.2°
      Damage threshold>10 J/cm2 at 1 ns
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    N. Jourdain, U. Chaulagain, M. Havlík, D. Kramer, D. Kumar, I. Majerová, V. T. Tikhonchuk, G. Korn, S. Weber. The L4n laser beamline of the P3-installation: Towards high-repetition rate high-energy density physics at ELI-Beamlines[J]. Matter and Radiation at Extremes, 2021, 6(1): 015401

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    Paper Information

    Category:

    Received: Jul. 17, 2020

    Accepted: Oct. 24, 2020

    Published Online: Apr. 22, 2021

    The Author Email: Weber S. (stefan.weber@eli-beams.eu)

    DOI:10.1063/5.0022120

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