• Matter and Radiation at Extremes
  • Vol. 9, Issue 3, 035201 (2024)
Zhongtao Xiang*, Changhai Yu, Zhiyong Qin, Xuhui Jiao..., Jiahui Cheng, Qiaoxuan Zhou, Gatie Axi, Jianghua Jie, Ya Huang, Jintan Cai and Jiansheng Liu|Show fewer author(s)
Author Affiliations
  • Department of Physics, Shanghai Normal University, Shanghai 200234, China
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    DOI: 10.1063/5.0189460 Cite this Article
    Zhongtao Xiang, Changhai Yu, Zhiyong Qin, Xuhui Jiao, Jiahui Cheng, Qiaoxuan Zhou, Gatie Axi, Jianghua Jie, Ya Huang, Jintan Cai, Jiansheng Liu. Ultrahigh-brightness 50 MeV electron beam generation from laser wakefield acceleration in a weakly nonlinear regime[J]. Matter and Radiation at Extremes, 2024, 9(3): 035201 Copy Citation Text show less
    (a) Schematic illustration of laser pulse propagation in a typical density-tailored plasma with three down-slope distributions, where Ld1, Ld2, and Ld3 represent the injection stage, acceleration stage, and transportation stage, respectively. (b) Evolution of normalized laser intensity and wake phase velocity in the plasma. (c)–(e) 3D views of TW laser-driven wakefield acceleration using FBPIC simulations, for three segments at t = 1.46, 1.93, and 3.11 ps, respectively.
    Fig. 1. (a) Schematic illustration of laser pulse propagation in a typical density-tailored plasma with three down-slope distributions, where Ld1, Ld2, and Ld3 represent the injection stage, acceleration stage, and transportation stage, respectively. (b) Evolution of normalized laser intensity and wake phase velocity in the plasma. (c)–(e) 3D views of TW laser-driven wakefield acceleration using FBPIC simulations, for three segments at t = 1.46, 1.93, and 3.11 ps, respectively.
    (a)–(c) Plasma density, longitudinal acceleration field, and trajectory of injected electrons at different times t = 1.40, 1.46, and 1.51 ps, respectively. (d) The e-beam energy spectrum at injection time t = 1.46 ps. (e) Corresponding transverse density distribution of e-beam (blue shading), focusing field (green curve), and transverse momentum distribution (orange shading). (f) Longitudinal velocity distribution (red curve) and observed longitudinal acceleration field (green curve) of e beam at t = 1.51 ps after Ld1.
    Fig. 2. (a)–(c) Plasma density, longitudinal acceleration field, and trajectory of injected electrons at different times t = 1.40, 1.46, and 1.51 ps, respectively. (d) The e-beam energy spectrum at injection time t = 1.46 ps. (e) Corresponding transverse density distribution of e-beam (blue shading), focusing field (green curve), and transverse momentum distribution (orange shading). (f) Longitudinal velocity distribution (red curve) and observed longitudinal acceleration field (green curve) of e beam at t = 1.51 ps after Ld1.
    Evolution of transverse position [(a) and (d)], transverse momentum [(b) and (e)], and emittance [(c) and (f)] of e beams for longitudinal injection in a weakly nonlinear LWFA [(a)–(c)], as compared with the transverse injection case for the bubble regime [(d)–(f)].
    Fig. 3. Evolution of transverse position [(a) and (d)], transverse momentum [(b) and (e)], and emittance [(c) and (f)] of e beams for longitudinal injection in a weakly nonlinear LWFA [(a)–(c)], as compared with the transverse injection case for the bubble regime [(d)–(f)].
    (a) Evolution of energy peak value (blue curve) and energy spread (red curve) during the acceleration stage Ld2 (blue shading) and transport stage Ld3 (yellow shading). (b) Energy spectra for different times t = 1.46 ps (black), 1.93 ps (blue), 2.50 ps (green), and 3.11 ps (red). (c)–(f) Corresponding electron phase spatial distribution, energy spectrum (orange shading), and charge current (blue shading). The inset in (f) shows the energy angular distribution of the e beam.
    Fig. 4. (a) Evolution of energy peak value (blue curve) and energy spread (red curve) during the acceleration stage Ld2 (blue shading) and transport stage Ld3 (yellow shading). (b) Energy spectra for different times t = 1.46 ps (black), 1.93 ps (blue), 2.50 ps (green), and 3.11 ps (red). (c)–(f) Corresponding electron phase spatial distribution, energy spectrum (orange shading), and charge current (blue shading). The inset in (f) shows the energy angular distribution of the e beam.
    (a) and (b) Charge (black curve) and energy (blue curve) as functions of the injection distance Ld1 and the peak density npeak. (c) and (d) Corresponding energy spread (black curve) and emittance (red curve). The blue shading corresponds to the case shown in Figs. 2 and 4.
    Fig. 5. (a) and (b) Charge (black curve) and energy (blue curve) as functions of the injection distance Ld1 and the peak density npeak. (c) and (d) Corresponding energy spread (black curve) and emittance (red curve). The blue shading corresponds to the case shown in Figs. 2 and 4.
    Zhongtao Xiang, Changhai Yu, Zhiyong Qin, Xuhui Jiao, Jiahui Cheng, Qiaoxuan Zhou, Gatie Axi, Jianghua Jie, Ya Huang, Jintan Cai, Jiansheng Liu. Ultrahigh-brightness 50 MeV electron beam generation from laser wakefield acceleration in a weakly nonlinear regime[J]. Matter and Radiation at Extremes, 2024, 9(3): 035201
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