Matter and Radiation at Extremes, Volume. 9, Issue 1, 016601(2024)

Nonstationary laser-supported ionization wave in layer of porous substance with subcritical density

S. Yu Gus’kov and R. A. Yakhina)
Author Affiliations
  • P.N. Lebedev Physical Institute of Russian Academy of Sciences, Leninskii Prospect 53, Moscow 119991, Russia
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    Figures & Tables(8)
    Pressure isoline distributions at moments of time 0.5, 1, and 1.3 ns (from left to right) after the beginning of the laser pulse. The porous layer initially occupies the area from 100 to 600 μm.
    Pressure (black line) and temperature (red line) distributions along the optical axis of the laser beam at the moment of time 1.3 ns. The porous layer initially occupies the area from 100 to 600 μm.
    Dependences of delay degree tp/tc (a) and ionization wave passage time tp (b) on layer thickness S at a laser intensity of 1014 W cm−2 for two wavelengths 0.53 μm (solid lines) and 0.35 μm (dotted lines) and for three densities 10 mg cm−3 (black lines), 5 mg cm−3 (red lines), and 2 mg cm−3 (green lines).
    Dependences of delay degree tp/tc (a) and ionization wave passage time tp (b) on layer thickness S at a laser intensity of 1015 W cm−2 for two wavelengths 0.53 μm (solid lines) and 0.35 μm (dotted lines) and for three densities 10 mg cm−3 (black lines), 5 mg cm−3 (red lines), and 2 mg cm−3 (green lines).
    Dependences of optimal pulse energy (a) and average ionization wave velocity (b) on layer thickness S at a laser intensity of 1014 W cm−2 for two wavelengths 0.53 μm (solid lines) and 0.35 μm (dotted lines) and for three densities 10 mg cm−3 (black lines), 5 mg cm−3 (red lines), and 2 mg cm−3 (green lines).
    Dependences of optimal pulse energy (a) and average ionization wave velocity (b) on layer thickness S at a laser intensity of 1015 W cm−2 for two wavelengths 0.53 μm (solid lines) and 0.35 μm (dotted lines) and for three densities 10 mg cm−3 (black lines), 5 mg cm−3 (red lines), and 2 mg cm−3 (green lines).
    • Table 1. Experimental conditions.a

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      Table 1. Experimental conditions.a

      ExperimentI (1014 W cm−2)τL (ns)λ (μm)R (μm)S (μm)ρ (mg cm−3)δ0 (μm)tex (ns)Dex (107cm s−1)Notes
      Gekko-1221330.3510050010∼11.72.9Normal incidence of
      LIL642.70.35100095010∼11.66third-harmonic Nd-laser beam
      PALS22,2340.320.441503804.5∼20.57.6Normal incidence of
      PALS22,2340.320.441504009∼21.33.1third-harmonic I-laser beam
      JLF24320.5310044212251.43.16Normal incidence of
      second-harmonic Nd-laser beam
      Shenguang III4–810.35250800/210–12∼13–3.5Oblique incidence of two beams of
      prototype25third-harmonic Nd-laser radiation
    • Table 2. Model results.a

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      Table 2. Model results.a

      1D solution2D model
      ExperimentDh (107cm s−1)Dca (107cm s−1)td (ns)tp (ns)Da (107cm s−1)Dh* (107cm s−1)Dca* (107cm s−1)td* (ns)tp* (ns)Dca*/Dh*Da* (107cm s−1)
      Gekko-126.612.50.550.766.436.81.571.672.33
      LIL8.111.20.621.536.26.89.70.671.91.65.1
      PALS (4.5 mg cm−3)15951.170.25159.8762.40.397.89.8
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    S. Yu Gus’kov, R. A. Yakhin. Nonstationary laser-supported ionization wave in layer of porous substance with subcritical density[J]. Matter and Radiation at Extremes, 2024, 9(1): 016601

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    Paper Information

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    Received: May. 12, 2023

    Accepted: Sep. 4, 2023

    Published Online: Mar. 27, 2024

    The Author Email: R. A. Yakhin (yakhin.rafael@gmail.com)

    DOI:10.1063/5.0157904

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