High Power Laser Science and Engineering, Volume. 13, Issue 4, 04000e65(2025)

Assessing optical damage risks by simulating the amplification of back-reflection in a multi-petawatt laser system

Dmitrii Nistor1,2, Alice Diana Dumitru1,2,3, Christophe Derycke4, Olivier Chalus4, Daniel Ursescu1,3, and Catalin Ticos1,2
Author Affiliations
  • 1Extreme Light Infrastructure - Nuclear Physics (ELI-NP), https://ror.org/048m5jb39Horia Hulubei National Institute of Physics and Nuclear Engineering, Măgurele, Romania
  • 2Engineering and Applications of Lasers and Accelerators Doctoral School (SDIALA), National University of Science and Technology Politehnica of Bucharest, Bucharest, Romania
  • 3Physics Doctoral School, https://ror.org/02x2v6p15University of Bucharest, Măgurele, Romania
  • 4Thales LAS France, Elancourt, France
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    Figures & Tables(9)
    Logic scheme of the framework that models the amplification chain. The AMP function gathers data from the input matrix and calls PASS to perform the calculation.
    Simplified cross-sectional view of Amp 1.2’s geometrical model, illustrating beam clipping and divergence evolution during amplification. The red area shows the main beam propagation, green represents the pump diameter and the yellow arrow indicates the propagation direction. Calculated attenuation values for each pass are 0.71, 0.47, 0.71, 0.95 and 1.24. Note that the reduced diameter in the final pass enhances the extraction efficiency.
    Map of gain decay (in percent) at the moment when the BR reaches each amplifier.
    Monitoring BR amplification across the HPLS for the presented scenarios. The order of amplifiers is in line with the propagation of BR light.
    Gain in the post-pulse regime in different pumping scenarios with their respective pumping energies. Note the residual gain is smaller in Amp 3.1 and Amp 3.2 for the full pump scenario due to the high extraction efficiency, despite being strongly pumped before the last pass. The order of amplifiers is in line with propagation of BR light.
    Normalized energy and spectral output of each amplifier in the chain. (a) Simulated amplification in the spectral domain. (b) Acquired spectra from each amplifier during the 10 PW experimental campaign. (c) Measured and simulated energy for each amplifier.
    Evolution of the BR spectrum across the simulated amplification chain traveling from Amp 3.2 to Amp 1.1 with a negative chirp.
    • Table 1. Fine-tuning parameters (green cells) for Amp 1.1 (blue cells) and Amp 1.2 (orange cells) using the optimization algorithm. The best parameter values obtained (highlighted in red) are passed down for later use in the full model of the amplification chain (Table 2).

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      Table 1. Fine-tuning parameters (green cells) for Amp 1.1 (blue cells) and Amp 1.2 (orange cells) using the optimization algorithm. The best parameter values obtained (highlighted in red) are passed down for later use in the full model of the amplification chain (Table 2).

    • Table 2. Obtained input parameters, which describe each amplifier in the HPLS.

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      Table 2. Obtained input parameters, which describe each amplifier in the HPLS.

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    Dmitrii Nistor, Alice Diana Dumitru, Christophe Derycke, Olivier Chalus, Daniel Ursescu, Catalin Ticos. Assessing optical damage risks by simulating the amplification of back-reflection in a multi-petawatt laser system[J]. High Power Laser Science and Engineering, 2025, 13(4): 04000e65

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    Paper Information

    Category: Research Articles

    Received: Apr. 9, 2025

    Accepted: Jun. 24, 2025

    Published Online: Sep. 24, 2025

    The Author Email:

    DOI:10.1017/hpl.2025.10049

    CSTR:32185.14.hpl.2025.10049

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