Laser Wakefield Accelerators

Najmudin, Z.

doi:10.5170/CERN-2016-001.109

Published Articles
Report number	arXiv:1705.10534
Title	Laser Wakefield Accelerators
Author(s)	Najmudin, Z. (JAI, UK ; Imperial Coll., London)
Publication	Geneva : CERN, 2016
Imprint	2017-05-30
Number of pages	10
Note	10 pages, contribution to the CAS - CERN Accelerator School: Plasma Wake Acceleration, CERN, Geneva, Switzerland, 23 - 29 Nov 2014
In:	CAS - CERN Accelerator School: Plasma Wake Acceleration, pp.109-118
DOI	10.5170/CERN-2016-001.109
Subject category	Accelerators and Storage Rings
Abstract	The one-dimensional wakefield generation equations are solved for increasing levels of non-linearity, to demonstrate how they contribute to the overall behaviour of a non-linear wakefield in a plasma. The effect of laser guiding is also studied as a way to increase the interaction length of a laser wakefield accelerator.
Copyright/License	publication: © 2016-2025 CERN (License: CC-BY-4.0)

$Linear wakefield generation: plots of $E/E_{0}$, $v/c$, and $n_\mathrm{e}/n_{0}$ (in blue) for laser pulse $a=a_{0}\sin(\pi \zeta/L)$ with pulse length $L= {\rm (a)}\, \frac{1}{2}, {\rm (b)}\, 1, {\rm (c)}\, 2 \, \lambda_\mathrm{p}$ and $a_{0} = 0.2$ (in red).$ $Linear wakefield generation: plots of $E/E_{0}$, $v/c$, and $n_\mathrm{e}/n_{0}$ (in blue) for laser pulse $a=a_{0}\sin(\pi \zeta/L)$ with pulse length $L= {\rm (a)}\, \frac{1}{2}, {\rm (b)}\, 1, {\rm (c)}\, 2 \, \lambda_\mathrm{p}$ and $a_{0} = 0.2$ (in red).$ $Linear wakefield generation: plots of $E/E_{0}$, $v/c$, and $n_\mathrm{e}/n_{0}$ (in blue) for laser pulse $a=a_{0}\sin(\pi \zeta/L)$ with pulse length $L= {\rm (a)}\, \frac{1}{2}, {\rm (b)}\, 1, {\rm (c)}\, 2 \, \lambda_\mathrm{p}$ and $a_{0} = 0.2$ (in red).$ Show more plots

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Zapis kreiran 2016-08-03, zadnja izmjena 2023-03-14

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