• High Power Laser and Particle Beams
  • Vol. 33, Issue 8, 081002 (2021)
Xiaoling Ji and Yu Deng
Author Affiliations
  • Department of Physics, Sichuan Normal University, Chengdu 610068, China
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    DOI: 10.11884/HPLPB202133.210211 Cite this Article
    Xiaoling Ji, Yu Deng. Research progress on self-focusing effect of high-power laser beams propagating in inhomogeneous atmosphere[J]. High Power Laser and Particle Beams, 2021, 33(8): 081002 Copy Citation Text show less
    Diagram of high-power laser beam propagating upwards in atmosphere[24]
    Fig. 1. Diagram of high-power laser beam propagating upwards in atmosphere[24]
    Confirmation of Eq. (4). Modified beam width wmod versus propagation distance z. Dashed curves: by Eq. (4); solid curves: by numerical simulation[24]
    Fig. 2. Confirmation of Eq. (4). Modified beam width wmod versus propagation distance z. Dashed curves: by Eq. (4); solid curves: by numerical simulation[24]
    Confirmation of Eq. (7). Beam width wtar ontarget versus relative power P/PcrGs[25]
    Fig. 3. Confirmation of Eq. (7). Beam width wtar ontarget versus relative power P/PcrGs[25]
    Beam width w versus the propagation distance z. Dashed lines: linear propagation in free space; Solid lines: nonlinear propagation in the atmosphere[23]
    Fig. 4. Beam width w versus the propagation distance z. Dashed lines: linear propagation in free space; Solid lines: nonlinear propagation in the atmosphere[23]
    Relative pulse width T/T0 versus propagation distance z[21]
    Fig. 5. Relative pulse width T/T0 versus propagation distance z[21]
    Intensity distributions I(x, y = 0, z) versus altitude z[33]
    Fig. 6. Intensity distributions I(x, y = 0, z) versus altitude z[33]
    Normalized intensity distributions I/I0 on debris target[21]
    Fig. 7. Normalized intensity distributions I/I0 on debris target[21]
    Intensity distribution I(r, z)versus propagation distance z. Uniform irradiation on debris target[22]
    Fig. 8. Intensity distribution Ir, z)versus propagation distance z. Uniform irradiation on debris target[22]
    (a) Intensity distribution I(r, z) and (b) phase distribution Ф(r, z) at the exit of the atmosphere, (c) relative intensity distribution I(r, z)/Ipeak on the target[22]
    Fig. 9. (a) Intensity distribution I(r, z) and (b) phase distribution Ф(r, z) at the exit of the atmosphere, (c) relative intensity distribution I(r, z)/Ipeak on the target[22]
    Intensity distributions for different values of obscure ratio ε on ground[33]
    Fig. 10. Intensity distributions for different values of obscure ratio ε on ground[33]
    Comparison of intensity distributions on debris target[21]
    Fig. 11. Comparison of intensity distributions on debris target[21]
    Beam width wtar on target versus focal length F[25]
    Fig. 12. Beam width wtar on target versus focal length F[25]
    Beam width on target versus wavelength λ[25]
    Fig. 13. Beam width on target versus wavelength λ[25]
    Optimal wavelength λopt versus lg(C0) and σ0[25]
    Fig. 14. Optimal wavelength λopt versus lg(C0) and σ0[25]
    Phase distribution [24]相位分布[24]
    Fig. 15. Phase distribution [24]相位分布 [24]
    Intensity distribution I(x, y, z) at different propagation distance z[24]
    Fig. 16. Intensity distribution I(x, y, z) at different propagation distance z[24]
    With PC, intensity distribution I(x, y, z) at different propagation distance z[24]
    Fig. 17. With PC, intensity distribution I(x, y, z) at different propagation distance z[24]
    Xiaoling Ji, Yu Deng. Research progress on self-focusing effect of high-power laser beams propagating in inhomogeneous atmosphere[J]. High Power Laser and Particle Beams, 2021, 33(8): 081002
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