2004
DOI: 10.1103/physreve.70.056410
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Simulation of ultrashort electron pulse generation from optical injection into wake-field plasma waves

Abstract: A laser-plasma-based source of relativistic electrons is described in detail, and analyzed in two dimensions using theoretical and numeric techniques. Two laser beams are focused in a plasma, one exciting a wake-field electron plasma wave while another locally alters some electron trajectories in such a way that they can be trapped and accelerated by the wave. Previous analyses dealt only with one-dimensional models. In this paper two-dimensional particle-in-cell simulations and analysis of single particle tra… Show more

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Cited by 18 publications
(6 citation statements)
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“…Electrons in group II originate directly on the axis of the drive pulse, and to the side of the injector pulse (yellow trajectory). These electrons first experience the interaction with the drive pulse, and then kicked and injected into the drive wakefield by the combination of the injector pulse's ponderomotive force and its wakefield [19,44,45]. This group is injected via ponderomotive drift and, partially, due to stochastic heating in the beatwave.…”
mentioning
confidence: 99%
“…Electrons in group II originate directly on the axis of the drive pulse, and to the side of the injector pulse (yellow trajectory). These electrons first experience the interaction with the drive pulse, and then kicked and injected into the drive wakefield by the combination of the injector pulse's ponderomotive force and its wakefield [19,44,45]. This group is injected via ponderomotive drift and, partially, due to stochastic heating in the beatwave.…”
mentioning
confidence: 99%
“…As the wake fields propagated forward, more and more electrons with energy above the trapping threshold were captured until the largest amplitude formation of the plasma wave. [24,25] As described in Ref. [2], wave breaking is not always catastrophic and a part of the electrons in the wave can escape, reducing its amplitude, while maintaining the wave structure.…”
Section: Nozzle Electronmentioning
confidence: 99%
“…Since the ponderomotive force is proportional to the laser intensity gradient, these pushed electrons were directed primarily in the longitudinal direction because the laser pulse length (𝑐𝜏 = 9 µm) is much shorter than its focal spot size in our experiment. [24] On the other hand, the ions do not respond to the ponderomotive force because their mass is much larger than electrons. Under the restoring force (backward and centripetal) due to the electric field of the space charge separation, the electrons would be dragged back towards their original position.…”
Section: Nozzle Electronmentioning
confidence: 99%
“…2) How can we capture enough electrons? There are several ways to "inject" the electrons into the plasma wave, such as wave-breaking injection [1,10], blow-out/bubble injection [11,12], external injection [13], optical injection [14], density transition injection [15], etc. Optical injection and density transition injection are complicated for an experimental setup and with regard to the technique today it is hard to externally inject the charged particles into a plasma wave with the wavelength of only several millimeters.…”
Section: Theoretical Backgroundsmentioning
confidence: 99%