2018
DOI: 10.1088/1361-6587/aab3b5
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Bremsstrahlung hard x-ray source driven by an electron beam from a self-modulated laser wakefield accelerator

Abstract: An x-ray source generated by an electron beam produced using a Self-Modulated Laser Wakefield Accelerator (SM-LWFA) is explored for use in high energy density science facilities. By colliding the electron beam, with a maximum energy of 380 MeV, total charge of >10 nC and a divergence of 64 × 100 mrad, from a SM-LWFA driven by a 1 ps 120 J laser, into a high-Z foil, an x/gamma-ray source was generated. A broadband bremsstrahlung energy spectrum with temperatures ranging from 0.8 to 2 MeV was measured with an al… Show more

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Cited by 42 publications
(40 citation statements)
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“…If the electron comes to a total stop, it transfers all its energy into the photon, therefore the maximum energy of the Gamma-ray beam matches the maximum energy of the electron beam. This configuration has been shown to work operating in the blowout LWFA regime [17] and in the self-modulated LWFA regime where it benefits from the almost one order of magnitude increased electron beam charge generating a larger number gamma photons [51]. It was found experimentally on the Vulcan facility, operating at 5 × 10 19 W/cm 2 , that the interaction of the laser pulse with a gas jet in front of a tantalum foil enhances the on-axis dose by a factor 5 with respect to interaction on a solid target and produces a gamma-ray lobe directed on-axis with a reduced angular spread [52].…”
Section: Alternative Plasma-based Gamma Ray Sourcesmentioning
confidence: 99%
“…If the electron comes to a total stop, it transfers all its energy into the photon, therefore the maximum energy of the Gamma-ray beam matches the maximum energy of the electron beam. This configuration has been shown to work operating in the blowout LWFA regime [17] and in the self-modulated LWFA regime where it benefits from the almost one order of magnitude increased electron beam charge generating a larger number gamma photons [51]. It was found experimentally on the Vulcan facility, operating at 5 × 10 19 W/cm 2 , that the interaction of the laser pulse with a gas jet in front of a tantalum foil enhances the on-axis dose by a factor 5 with respect to interaction on a solid target and produces a gamma-ray lobe directed on-axis with a reduced angular spread [52].…”
Section: Alternative Plasma-based Gamma Ray Sourcesmentioning
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%
“…Today however, bright electron beams with GeV energies can be produced over a few centimetres by laser wakefield acceleration (LWFA) [5,6]. These electron beams can be used to produce brilliant γ ray beams by bremsstrahlung [7,8,9,10] and inverse Compton scattering [11,12,13]. Colliding such brilliant γ ray photons with a suitable x-ray photon field could be a viable route to study two-photon physics in the laboratory for the first time [14,15].…”
Section: Introductionmentioning
confidence: 99%