High Power Laser Science and Engineering, Volume. 8, Issue 4, 04000e43(2020)

High-energy hybrid femtosecond laser system demonstrating 2 × 10 PW capability On the Cover

François Lureau1, Guillaume Matras1, Olivier Chalus1, Christophe Derycke1, Thomas Morbieu1, Christophe Radier1, Olivier Casagrande1, Sébastien Laux1, Sandrine Ricaud1, Gilles Rey1, Alain Pellegrina1, Caroline Richard1, Laurent Boudjemaa1, Christophe Simon-Boisson1, Andrei Baleanu2, Romeo Banici2, Andrei Gradinariu2, Constantin Caldararu2, Bertrand De Boisdeffre3, Petru Ghenuche3, Andrei Naziru3,4, Georgios Kolliopoulos3, Liviu Neagu3, Razvan Dabu3, Ioan Dancus3、*, and Daniel Ursescu3
Author Affiliations
  • 1Thales LAS France, 78990Élancourt, France
  • 2Thales Systems Romania, 060071București, Romania
  • 3Extreme Light Infrastructure – Nuclear Physics, ‘Horia Hulubei’ National Institute for Physics and Nuclear Engineering, 077125Bucharest Magurele, Romania
  • 4University of Bucharest, Faculty of Physics, 077125Bucharest Magurele, Romania
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    Figures & Tables(24)
    Block diagram of FE and one amplification arm with the three corresponding outputs: 100 TW at 10 Hz, 1 PW at 1 Hz, and 10 PW at 1 shot/min repetition rate.
    Venteon oscillator spectrum.
    CPA1 and XPW spectra.
    Near-field spatial intensity profile of the picosecond pulses: (a) before beam shaping device; (b) after beam shaping device.
    Near-field beam intensity profile of the 532 nm picosecond pump laser for OPCPA.
    Evolution of the 800 nm broadband beam spatial intensity profile through the FE. The FE near-field intensity and far-field intensity profiles were measured at the output of the second OPCPA stage.
    Stability of the OPCPA spectrum over 7 h continuous operation. The red curve is the average of the data acquired at 10 min intervals that we represented by the gray curves.
    FE contrast assessment. By blocking the device input, the limitation of the measurement device sensitivity has been evaluated in the range of 10–13.
    The typical beam profile of the pump lasers.
    Pulse temporal profile of the ATLAS 100 laser, 50 ns/div; delay between laser pulses was set at 50 ns; the entire FWHM pulse duration, for combined pulses, is about 70 ns.
    The beam profile at the output of each main amplifier.
    Schematic configuration of the high-energy Ti:sapphire amplification arm.
    Spectral bandwidth management through the high-energy Ti:sapphire amplifiers: (a) typical reflectivity and dispersion of the spectral filters at 45° angle of incidence; (b) simulation of 100 μJ energy, Gaussian spectrum seed pulse (blue line) propagation through five chirped pulse amplifiers to reach 90 J output pulse energy, with spectral shaping mirrors (gray line) and without spectral shaping mirrors (red line).
    Evolution of the spectrum through the high-power Ti:sapphire amplifiers
    The HPLS 10 PW compressor and diagnostics diagram; the inset is a picture of one of the two ELI-NP 10 PW compressors using the meter size gratings. D.M., deformable mirror; WFS, wavefront sensor; CCD-NF, near-field CCD; CCD-FF, far-field CCD; AUTO-CO, single-shot autocorrelator; CROSS-CO, third-order cross-correlator.
    Extraction efficiency for the 10 PW level amplifier AMP3.2.
    Wizzler measurements: (a) flat spectral phase and more than 70 nm spectral bandwidth; (b) reconstructed pulse with τ = 22.7 FWHM duration.
    Contrast measurements at the output of the HPLS for the different amplification levels.
    Measured data from the wavefront sensor and far-field camera on the 10 PW diagnostic bench. The wavefront map shows a wavefront error of 0.05 μm RMS. The calculated PSF from the measured irradiance map and wavefront map shows an SR of 0.9. Far-field profile confirms the good focusability of the beam.
    Long-term stability test for the 1 PW level amplifier during 1 day of operation showing the energy of all the shots before compression.
    • Table 1. Main beam parameters at each amplification level during the 10 PW operation.

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      Table 1. Main beam parameters at each amplification level during the 10 PW operation.

      InputUsed/availableOutputEnergyBeam
      AMPenergypump energyenergystabilitysize
      AMP1.10.5 mJ110 mJ/200 mJ25 mJ< 3% RMS2 mm
      AMP1.225 mJ11 J/14.2 J3.5 J< 3% RMS28 mm
      AMP22 J85 J/96 J35 J< 2% RMS55 mm
      AMP3.120 J180 J/200 J80 J< 2% RMS90 mm
      AMP3.280 J480 J/600 J327 J< 1.8% RMS130 mm
    • Table 2. Beam size and deformable mirror characteristics.

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      Table 2. Beam size and deformable mirror characteristics.

      100 TW1 PW10 PW
      Beam size at the deformable mirror28 mm55 mm130 mm
      Deformable mirror size50 mm100 mm180 mm
      Optimum beam diameter for correction20–30 mm40–60 mm125–180 mm
      Number of actuators254358
    • Table 3. Measured parameters of the HPLS.

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      Table 3. Measured parameters of the HPLS.

      Output type100 TW1 PW10 PW
      Pulse energy (J)a2.725243
      Pulse duration (fs)b<25<24<23
      Repetition rate (Hz)1011/60
      Calculated SR from measured wavefront>0.9>0.9>0.9
      Pointing stability (μrad RMS)c<3.4<1.78<1.27
      Pulse energy stability (RMS)c<2.6%<1.8%<1.8%
      FE demonstrated ps contrastdIn the range of 1013:1
    • Table 4. Stability test for the 10 PW level amplifier running for 90 min at 300 J.

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      Table 4. Stability test for the 10 PW level amplifier running for 90 min at 300 J.

      ParameterValue
      Average value300.5 J
      Maximum value305 J
      Minimum value254 J
      RMS stability1.798%
      Point-to-point stability17.14%
      Standard deviation5.4 J
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    François Lureau, Guillaume Matras, Olivier Chalus, Christophe Derycke, Thomas Morbieu, Christophe Radier, Olivier Casagrande, Sébastien Laux, Sandrine Ricaud, Gilles Rey, Alain Pellegrina, Caroline Richard, Laurent Boudjemaa, Christophe Simon-Boisson, Andrei Baleanu, Romeo Banici, Andrei Gradinariu, Constantin Caldararu, Bertrand De Boisdeffre, Petru Ghenuche, Andrei Naziru, Georgios Kolliopoulos, Liviu Neagu, Razvan Dabu, Ioan Dancus, Daniel Ursescu. High-energy hybrid femtosecond laser system demonstrating 2 × 10 PW capability[J]. High Power Laser Science and Engineering, 2020, 8(4): 04000e43

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    Paper Information

    Category: Research Articles

    Received: Aug. 1, 2020

    Accepted: Oct. 26, 2020

    Published Online: Jan. 5, 2021

    The Author Email: Ioan Dancus (ioan.dancus@eli-np.ro)

    DOI:10.1017/hpl.2020.41

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