• Matter and Radiation at Extremes
  • Vol. 8, Issue 1, 014403 (2023)
Yuan Zhao1、2、3, Haiyang Lu1、2, Cangtao Zhou1、2、3, and Jungao Zhu1、2
Author Affiliations
  • 1Center for Advanced Material Diagnostic Technology and College of Engineering Physics, Shenzhen Technology University, Shenzhen 518118, People’s Republic of China
  • 2Shenzhen Key Laboratory of Ultraintense Laser and Advanced Material Technology, Shenzhen Technology University, Shenzhen 518118, People’s Republic of China
  • 3College of Optoelectronic Engineering, Shenzhen University, Shenzhen 518060, People’s Republic of China
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    DOI: 10.1063/5.0121558 Cite this Article
    Yuan Zhao, Haiyang Lu, Cangtao Zhou, Jungao Zhu. Overcritical electron acceleration and betatron radiation in the bubble-like structure formed by re-injected electrons in a tailored transverse plasma[J]. Matter and Radiation at Extremes, 2023, 8(1): 014403 Copy Citation Text show less
    (a) The phase differences of the plasma wave after 20T0 passage in a transversely tailored plasma (red solid line) and a uniform plasma (black solid line). The spatial distribution of the transverse magnetic field Bz (b) and the backward electron density (c) at 20T0. (d) A few typical trajectories of the re-injected electrons.
    Fig. 1. (a) The phase differences of the plasma wave after 20T0 passage in a transversely tailored plasma (red solid line) and a uniform plasma (black solid line). The spatial distribution of the transverse magnetic field Bz (b) and the backward electron density (c) at 20T0. (d) A few typical trajectories of the re-injected electrons.
    The spatial distribution of the longitudinal electrostatic field (a) and the transverse field Eys − cBzs in the (x, y) plane (b) at 20T0. The black dashed box marks the position of the bubble.
    Fig. 2. The spatial distribution of the longitudinal electrostatic field (a) and the transverse field EyscBzs in the (x, y) plane (b) at 20T0. The black dashed box marks the position of the bubble.
    (a) The Hamiltonian and (b) the electron density distribution in phase space (ψ, γ). The terms in (6) are normalized with the simulation results for the fields and the electron motion. It follows that eEL/meω0c = 50, eESx/meω0c = 9.32, kE=eESy/meω02=1, kB=eBSzc/meω02=1.47, vy = 0.2, and vx = 0.98.
    Fig. 3. (a) The Hamiltonian and (b) the electron density distribution in phase space (ψ, γ). The terms in (6) are normalized with the simulation results for the fields and the electron motion. It follows that eEL/meω0c = 50, eESx/meω0c = 9.32, kE=eESy/meω02=1, kB=eBSzc/meω02=1.47, vy = 0.2, and vx = 0.98.
    (a) The spatial distribution of the plasma electron density at 32T0. (b) and (c) are plots of the on-axis longitudinal electric field Ex and the transverse field Ey − cBz, respectively. (d) The trajectory of a sample electron and the electromagnetic field that the electron experiences. (e) The evolution of the transverse and longitudinal momenta, normalized by mec, for the same electron. (f) The work done by the longitudinal and transverse fields. The two vertical dashed black lines in (a)–(c) mark the acceleration zone. The first and second vertical dashed lines in (d)–(f) show the start of the betatron resonance acceleration, while the third dashed line marks the end of the wake-field acceleration. The horizontal dashed line in (b)–(f) gives the zero value of the corresponding quantity.
    Fig. 4. (a) The spatial distribution of the plasma electron density at 32T0. (b) and (c) are plots of the on-axis longitudinal electric field Ex and the transverse field EycBz, respectively. (d) The trajectory of a sample electron and the electromagnetic field that the electron experiences. (e) The evolution of the transverse and longitudinal momenta, normalized by mec, for the same electron. (f) The work done by the longitudinal and transverse fields. The two vertical dashed black lines in (a)–(c) mark the acceleration zone. The first and second vertical dashed lines in (d)–(f) show the start of the betatron resonance acceleration, while the third dashed line marks the end of the wake-field acceleration. The horizontal dashed line in (b)–(f) gives the zero value of the corresponding quantity.
    (a) The phase space x–px of electrons inside the bubble at 32T0. (b) The longitudinal distribution of the electron density at the position with peak electron density. (c) The angular energy of the accelerated electrons. (d) The spectrum of the first electron microbunch.
    Fig. 5. (a) The phase space xpx of electrons inside the bubble at 32T0. (b) The longitudinal distribution of the electron density at the position with peak electron density. (c) The angular energy of the accelerated electrons. (d) The spectrum of the first electron microbunch.
    (a) The emitted photon density at 32T0. (b) The evolutions of the local electron oscillation period (black solid line) and the local strength parameter K(red solid line). (c) The angle energy of the generated photons. (d) The spectrum of photons emitted by the first electron bunch.
    Fig. 6. (a) The emitted photon density at 32T0. (b) The evolutions of the local electron oscillation period (black solid line) and the local strength parameter K(red solid line). (c) The angle energy of the generated photons. (d) The spectrum of photons emitted by the first electron bunch.
    (0.5 mm) parametersValues
    Lasers
    Laser intensity I05 × 1021 W cm−2
    Laser wavelength λ0μm
    Laser period T03.33 fs
    Waist radius of laser beam σµm
    Full duration at half maximum 2ln2τL39.2 fs
    Target
    MaterialAluminum
    Electron density ne02nc
    Plasma length L035 µm
    Initial electron temperature Te10 eV
    Table 1. Simulation parameters.
    Yuan Zhao, Haiyang Lu, Cangtao Zhou, Jungao Zhu. Overcritical electron acceleration and betatron radiation in the bubble-like structure formed by re-injected electrons in a tailored transverse plasma[J]. Matter and Radiation at Extremes, 2023, 8(1): 014403
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