EPJ Web of Conferences
Volume 59, 2013IFSA 2011 – Seventh International Conference on Inertial Fusion Sciences and Applications
|Number of page(s)||4|
|Section||XVII. Ultra-High Intensity Laser-Matter Interaction|
|Published online||15 November 2013|
Channeling of relativistic laser pulses in underdense plasmas and subsequent electron acceleration
1 Theoretical Physics Institute, University of Alberta, Edmonton T6G 2J1, Alberta, Canada
2 Centre de Physique Théorique, CNRS, Ecole Polytechnique, 91128 Palaiseau Cedex, France
3 P. N. Lebedev Physics Institute, Russian Academy of Science, Moscow 119991, Russia
4 Department of Physics, University of Ottawa, Ottawa, Ontario, Canada
a e-mail: email@example.com
Published online: 15 November 2013
This contribution is concerned with the nonlinear behavior of a relativistic laser pulse focused in an underdense plasma and with the subsequent generation of fast electrons. Specifically, we study the interaction of laser pulses having their intensity Iλ2 in the range [1019, 1020] W/cm2 μm2, focused in a plasma of electron density n0 such that the ratio n0/nc lies in the interval [10−3, 2 × 10−2], nc denoting the critical density; the laser pulse power PL exceeds the critical power for laser channeling Pch. The laser-plasma interaction in such conditions is investigated by means of 3D Particle in Cell (PIC) simulations. It is observed that the laser front gives rise to the excitation of a surface wave which propagates along the sharp boundaries of the electron free channel created by the laser pulse. The mechanism responsible for the generation of the fast electrons observed in the PIC simulations is then analyzed by means of a test particles code. It is thus found that the fast electrons are generated by the combination of the betatron process and of the acceleration by the surface wave. The maximum electron energy observed in the simulations with Iλ2 = 1020 W/cm2 μm2 and n0/nc = 2 × 10−2 is 350 MeV.
© Owned by the authors, published by EDP Sciences, 2013
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