Abstract

We studied the generation of low emittance high current monoenergetic beams from plasma waves driven by ultrashort laser pulses, in view of achieving beam brightness of interest for free-electron laser (FEL) applications. The aim is to show the feasibility of generating nC charged beams carrying peak currents much higher than those attainable with photoinjectors, together with comparable emittances and energy spread, compatibly with typical FEL requirements. We identified two regimes: the first is based on a laser wakefield acceleration plasma driving scheme on a gas jet modulated in areas of different densities with sharp density gradients. The second regime is the so-called bubble regime, leaving a full electron-free zone behind the driving laser pulse: with this technique peak currents in excess of 100 kA are achievable. We have focused on the first regime, because it seems more promising in terms of beam emittance. Simulations carried out using VORPAL show, in fact, that in the first regime, using a properly density modulated gas jet, it is possible to generate beams at energies of about 30 MeV with peak currents of 20 kA, slice transverse emittances as low as 0.3 mm mrad, and energy spread around 0.4%. These beams break the barrier of ${10}^{18}\text{ }\text{ }\mathrm{A}/(\mathrm{mm}\text{ }\mathrm{mrad}{)}^{2}$ in brightness, a value definitely above the ultimate performances of photoinjectors, therefore opening a new range of opportunities for FEL applications. A few examples of FELs driven by such kind of beams injected into laser undulators are finally shown. The system constituted by the electron beam under the effect of the electromagnetic undulator has been named AOFEL (for all optical free-electron laser).

Highlights

  • A few authors proposed to use plasma injectors as an electron beam driver for the self-amplified spontaneous emission (SASE) x-ray free-electron laser (FEL): the aim is to design and build compact FELs, taking advantage from the capability of plasma accelerators to produce GeV beams on mm-scale lengths, to be compared to km based rf linacs

  • In this paper we present a different approach, which has in common the goal to use a plasma injector to drive a compact SASE FEL, but differing in the type of regime used in the plasma channel to generate the electron beam and in the energy of the beam itself, which is in the range of a few tens of MeV instead of a few GeV

  • If the e.m. laser pulse is of the same wavelength of the laser pulse driving the plasma wave, the electron beam does not even need to be extracted from the plasma channel, and the FEL can be driven in absence of space charge effects at all

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Summary

INTRODUCTION

A few authors proposed to use plasma injectors as an electron beam driver for the self-amplified spontaneous emission (SASE) x-ray free-electron laser (FEL): the aim is to design and build compact FELs, taking advantage from the capability of plasma accelerators to produce GeV beams on mm-scale lengths, to be compared to km based rf linacs. In this paper we present a different approach, which has in common the goal to use a plasma injector to drive a compact SASE FEL, but differing in the type of regime used in the plasma channel to generate the electron beam and in the energy of the beam itself, which is in the range of a few tens of MeV instead of a few GeV To this purpose the use of an electromagnetic undulator, i.e., a counterpropagating laser pulse of proper wavelength, is foreseen, as recently proposed [2,3]. If the e.m undulator is made out of a CO2 laser pulse, while the plasma density is larger than 1019 cmÿ, it cannot propa-

E-BEAM GENERATION VIA LWFA
FEL SIMULATIONS
Findings
CONCLUSIONS
Full Text
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