Jul 2 – 6, 2018
Žofín Palace
Europe/Prague timezone

P5.2018 Launching electromagnetic cascades in high-intensity laser fields

Jul 6, 2018, 2:00 PM
2h
Mánes

Mánes

Speaker

Thomas George Blackburn

Description

See the full Abstract at http://ocs.ciemat.es/EPS2018ABS/pdf/P5.2018.pdf Launching electromagnetic cascades in high-intensity laser fields T. G. Blackburn1 , A. Ilderton2 , S. P. D. Mangles3 , C. D. Murphy4 , C. P. Ridgers4 , M. Marklund1 1 Department of Physics, Chalmers University of Technology, Gothenburg, Sweden 2 Centre for Mathematical Sciences, Plymouth University, Plymouth, UK 3 The John Adams Institute for Accelerator Science, Imperial College London, London, UK 4 York Plasma Institute, Department of Physics, University of York, York, UK A cascade of photon emission and electron-positron pair creation is launched when a high- energy electron or photon traverses a region of sufficiently strong electromagnetic field, such as at the focus of a high-power laser. Cascades in the highly nonlinear regime, where the laser strength parameter a0 1 and the quantum parameter χ ∼ 1, are relevant to the study of astrophysical plasmas, such as in pulsar magnetospheres, and will be a ubiquitous feature of high-intensity experiments at the next generation of laser facilities. When combined with the ultrarelativistic, ultrashort electron beams available from laser-wakefield acceleration, today’s high-intensity lasers have the capability to probe this regime, where the recoil from emission of multiple photons (radiation reaction) dominates the electron dynamics [1, 2]. If the fields are strong enough that χ ∼ 1, the photons will produce electron-positron pairs, and the daughter electrons and positrons will lose energy to secondary radiation. We discuss the prospects for observation of such a cascade in two experimental geometries: one in which a multi-GeV, laser-wakefield accelerated electron beam collides directly with a laser pulse, pro- ducing photons via nonlinear Compton scattering [3]; and one in which the electron beam first collides with a high-Z foil, producing GeV photons via bremsstrahlung that go on to collide with a high-intensity laser pulse [4]. References [1] J. M. Cole et al., Experimental Evidence of Radiation Reaction in the Collision of a High-Intensity Laser Pulse with a Laser-Wakefield Accelerated Electron Beam, Phys. Rev. X 8, 011020 (2018) [2] K. Poder et al., Evidence of strong radiation reaction in the field of an ultra-intense laser, arXiv:1709:01861 (2017) [3] T. G. Blackburn, A. Ilderton, C. D. Murphy and M. Marklund, Scaling laws for positron production in laser– electron-beam collisions, Phys. Rev. A 96, 022128 (2017) [4] T. G. Blackburn and M. Marklund, Nonlinear Breit-Wheeler pair creation with bremsstrahlung γ rays, arXiv:1802.06612 (2018)

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