Matter and Radiation at Extremes, Volume. 9, Issue 5, 057402(2024)

Rescattering of stimulated Raman side scattering in nonuniform plasmas

S. Tan1... Q. Wang2, Y. Chen3, W. B. Yao1, C. Z. Xiao1,a) and J. F. Myatt4 |Show fewer author(s)
Author Affiliations
  • 1School of Physics and Electronics, Hunan University, Changsha 410082, China
  • 2Institute of Applied Physics and Computational Mathematics, Beijing 100094, China
  • 3School of Electrical and Information Engineering, Anhui University of Science and Technology, Huainan, Anhui 232001, China
  • 4Department of Electrical and Computer Engineering, University of Alberta, 9211 116 St. NW, Edmonton, Alberta T6G 1H9, Canada
  • show less
    Figures & Tables(9)
    (a) Schematic of stimulated Raman side scattering (SRSS) and its rescattering in an inhomogeneous plasma. (b) Wave vector matching condition of first-order SRSS. (c) Wave vector matching condition of second-order rescattering of SRSS.
    (a) Spectrum of Ez(x, ky) in x–ky space averaged over 2 ps. The red dashed vertical line indicates a density ne = 0.11nc. (b) The corresponding spectrum Ez(kx, ky) in wave vector (kx–ky) space. (c) Spectrum of EPWs Ex(kx, ky) overlaid with wave vector matching conditions. (d) Blow-up of the region outlined by the red dashed rectangle in (c). These are Fourier spectra of real quantities, and so they are symmetric in k.
    Frequency–wave vector spectrum of light waves Ez(ky, ω) at ne = 0.09nc over the interval t = [1.4 ps, 1.5 ps].
    Growth of scattered light amplitudes over time. The red, green, and blue dots are the relative scattered light amplitudes E of first SRSS at n = 0.09nc, n = 0.12nc, and n = 0.15nc, respectively. The red plus signs are the relative scattered light amplitudes E of second SRSS at n = 0.09nc.
    (a) and (b) Electron distribution functions in momentum space at t = 1 and 2 ps, respectively. The red and yellow arrows indicate the EPW directions of the first- and second-order SRSS, respectively. (c) and (d) Electron distribution functions in x–px phase space at the corresponding times. (e) and (f) Electron distribution functions in x–py phase space at the corresponding times.
    Evolution of energy spectra along the propagation directions of the first- and second-order EPWs.
    (a)–(d) Ez(x, ky) averaged over 2 ps for pump intensities I = 1 × 1014 W/cm2, 5 × 1014 W/cm2, 1 × 1015 W/cm2, and 1 × 1016 W/cm2, respectively. The density scale length at 0.2nc is L = 400 μm and the electron temperature is Te = 2 keV.
    (a)–(d) Ez(x, ky) averaged over 2 ps for density scale lengths at 0.2nc of L = 100, 200, 400, and 800 μm, respectively. The pump intensity is I = 1 × 1015 W/cm2 and the electron temperature is Te = 2 keV.
    (a)–(d) Ez(x, ky) averaged over 2 ps for electron temperatures Te = 1, 2, 5, and 10 keV, respectively. The pump intensity is I = 1 × 1015 W/cm2 and the density scale length at 0.2nc is L = 400 μm.
    Tools

    Get Citation

    Copy Citation Text

    S. Tan, Q. Wang, Y. Chen, W. B. Yao, C. Z. Xiao, J. F. Myatt. Rescattering of stimulated Raman side scattering in nonuniform plasmas[J]. Matter and Radiation at Extremes, 2024, 9(5): 057402

    Download Citation

    EndNote(RIS)BibTexPlain Text
    Save article for my favorites
    Paper Information

    Category:

    Received: Mar. 4, 2024

    Accepted: Jul. 9, 2024

    Published Online: Oct. 14, 2024

    The Author Email: Xiao C. Z. (xiaocz@hnu.edu.cn)

    DOI:10.1063/5.0206740

    Topics