2020
DOI: 10.1016/j.hedp.2020.100859
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Electron beam and betatron x-ray generation in a hybrid electron accelerator driven by high intensity picosecond laser pulses

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Cited by 4 publications
(4 citation statements)
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“…Moreover, tens of nC directional electron beams can be produced from vacuum laser acceleration [26][27][28] or target surface electron acceleration [29] by laser-solid interactions, but an important limiting factor is the short acceleration distance resulting in electron energies that are usually less than 10 MeV. There is another method called self-modulated laser wakefield acceleration (SM-LWFA) [30][31][32][33] in which long laser pulses overlap with several tens of plasma waves, thereby trapping a large number of electrons and accelerating them in every wakefield, and the beam charge can be increased tremendously to hundreds of nC, [34,35] but this method requires a kilojoule-class picosecond (ps) laser facility with a size and cost that are at least ten times that of a fs laser facility. In general, for laser plasma electron acceleration using a small laser, it is a great challenge to realize an electron beam with a large charge, tight collimation and high energy.…”
Section: Introductionmentioning
confidence: 99%
“…Moreover, tens of nC directional electron beams can be produced from vacuum laser acceleration [26][27][28] or target surface electron acceleration [29] by laser-solid interactions, but an important limiting factor is the short acceleration distance resulting in electron energies that are usually less than 10 MeV. There is another method called self-modulated laser wakefield acceleration (SM-LWFA) [30][31][32][33] in which long laser pulses overlap with several tens of plasma waves, thereby trapping a large number of electrons and accelerating them in every wakefield, and the beam charge can be increased tremendously to hundreds of nC, [34,35] but this method requires a kilojoule-class picosecond (ps) laser facility with a size and cost that are at least ten times that of a fs laser facility. In general, for laser plasma electron acceleration using a small laser, it is a great challenge to realize an electron beam with a large charge, tight collimation and high energy.…”
Section: Introductionmentioning
confidence: 99%
“…There are also some efforts in improving beam charge by increasing laser energy and using high-Z gas [23][24][25][26], but they still do not break through the limitation of beam loading effect. While self-modulated laser wakefield acceleration (SM-LWFA) [27][28][29][30] that long laser pulse overlaps with several tens of plasma waves, large number of electrons can be trapped and accelerated in every wakefield and the beam charge can be increased tremendously to tens of nC [31,32], but it requires a hundred joule class picosecond (ps) laser facility. Moreover, directional electron beams with tens of nC charge have also been produced via vacuum laser acceleration with a plasma mirror injector [33,34].…”
Section: Introductionmentioning
confidence: 99%
“…Continued improvement of x-ray sources coupled to HEDS drivers is a constant priority at these facilities for backlighting and radiography. LPA-based x-ray sources utilizing self-modulated laser wakefield acceleration (SMLWFA) have already shown promise as MeV-class radiography or high-flux broadband sources 1 10 . SMLWFA-based sources can deliver such high fluxes on account of the two orders of magnitude higher electron charge that they deliver compared to other LPA sources (Fig.…”
Section: Introductionmentioning
confidence: 99%