2013
DOI: 10.1063/1.4819718
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Numerical modeling of multi-GeV laser wakefield electron acceleration inside a dielectric capillary tube

Abstract: Numerical modeling of laser wakefield electron acceleration inside a gas filled dielectric capillary tube is presented. Guiding of a short pulse laser inside a dielectric capillary tube over a long distance (∼1 m) and acceleration of an externally injected electron bunch to ultra-relativistic energies (∼5-10 GeV) are demonstrated in the quasi-linear regime of laser wakefield acceleration. Two dimensional axisymmetric simulations were performed with the code WAKE-EP (Extended Performances), which allows computa… Show more

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Cited by 22 publications
(18 citation statements)
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“…Particle-In-Cell codes (WAKE-EP 24 and Calder-Circ 25 ) were used to model the propagation of the NIR pulse throughout the plasma channel 20 . The resulting 3D electron density and Kr 8+ abundance were fed to our 3D Maxwell-Bloch code Dagon 21 .…”
Section: Simulationsmentioning
confidence: 99%
“…Particle-In-Cell codes (WAKE-EP 24 and Calder-Circ 25 ) were used to model the propagation of the NIR pulse throughout the plasma channel 20 . The resulting 3D electron density and Kr 8+ abundance were fed to our 3D Maxwell-Bloch code Dagon 21 .…”
Section: Simulationsmentioning
confidence: 99%
“…Metal capillaries can be considered as a special case of plasma-walled capillaries, as the metal walls behave like a cold dense plasma with a sharp boundary. Laser propagation in dielectric capillaries is understood quite well [20,21], and experimental observations agree with the theory [13,22]. Plasma-walled capillaries are more difficult for theoretical analysis, the available theory [23][24][25] is not experimentally verified yet, the experiments were performed in the sub-picosecond regime [10,18,19], and no experimental data are available for femtosecond pulses.…”
mentioning
confidence: 84%
“…Ingenious laser-plasma experiments have been set up, demonstrating first the possibility to accelerate electrons to hundreds of MeV [3,4,5], then to the symbolic threshold of 1 GeV [6], and then to 2 [7], 3 [8], 4 [9], and very recently 8 GeV [10]. These experimental results are supported by simulations with 3D particle-in-cell (PIC) codes, which further explore the acceleration up to 10 GeV [11], hundreds of GeV [12], or even 1 TeV [13], assuming the achievement of a good enough electron injection. Those experimental and theoretical results have been obtained with a certain care about either the charge or else the beam quality in terms of energy dispersion and emittance, but the latter are still far from those obtained in rf accelerators.…”
Section: Introductionmentioning
confidence: 92%