High Power Laser Science and Engineering, Volume. 8, Issue 4, 04000e38(2020)

Asymmetric pulse effects on pair production in polarized electric fields

Obulkasim Olugh1,2, Zi-Liang Li3, and Bai-Song Xie1,4、*
Author Affiliations
  • 1Key Laboratory of Beam Technology of the Ministry of Education, and College of Nuclear Science and Technology, Beijing Normal University, Beijing100875, China
  • 2Xinjiang Police College, Urumqi830011, China
  • 3School of Science, China University of Mining and Technology, Beijing100083, China
  • 4Beijing Radiation Center, Beijing100875, China
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    Figures & Tables(9)
    Momentum spectra of produced pairs for linear polarization () at in the plane when the rising pulse length is fixed but the falling pulse length becomes shorter with . The chosen parameters are , and , where is the electron mass.
    Same as Figure1 except that the falling pulse length becomes longer with .
    Same as Figure1 except for elliptic polarization, .
    Same as Figure2 except for elliptic polarization, .
    Same as Figure1 except for circular polarization, .
    Same as Figure 2 except for circular polarization, .
    The number density (in units of ) of pairs produced in differently polarized electric fields for the shorter falling length of the asymmetric pulse shape with . The field parameters are the same as in Figure 1. Here LP, EP and CP with squares, circles and triangles denote the linear , elliptical and circular cases, respectively.
    Same as Figure 7 except for the elongated falling case with .
    • Table 1. The peak values of the particle distribution function for the typical polarization when the rising pulse length is fixed and the falling pulse length is short and/or elongated. Note that these peaks occur at different values of the momentum .

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      Table 1. The peak values of the particle distribution function for the typical polarization when the rising pulse length is fixed and the falling pulse length is short and/or elongated. Note that these peaks occur at different values of the momentum .

      ${f}_{\mathrm{max}}\left(\mathbf{q},\infty \right)$ at peak
      $k=1$ $k=0.1$ $k=10$
      $\delta =0$ $29.40\times {10}^{-6}$ $8.28\times {10}^{-4}$ $5.24\times {10}^{-5}$
      $\delta =0.5$ $9.65\times {10}^{-6}$ $7.50\times {10}^{-4}$ $6.36\times {10}^{-5}$
      $\delta =1$ $2.36\times {10}^{-6}$ $6.46\times {10}^{-4}$ $6.38\times {10}^{-5}$
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    Obulkasim Olugh, Zi-Liang Li, Bai-Song Xie. Asymmetric pulse effects on pair production in polarized electric fields[J]. High Power Laser Science and Engineering, 2020, 8(4): 04000e38

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    Paper Information

    Category: Research Articles

    Received: Jul. 1, 2020

    Accepted: Aug. 31, 2020

    Posted: Sep. 2, 2020

    Published Online: Nov. 23, 2020

    The Author Email: Bai-Song Xie (bsxie@bnu.edu.cn)

    DOI:10.1017/hpl.2020.36

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