2006
DOI: 10.1103/physrevlett.96.165003
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Observation of a Fast Electron Beam Emitted along the Surface of a Target Irradiated by Intense Femtosecond Laser Pulses

Abstract: A novel fast electron beam emitting along the surface of a target irradiated by intense laser pulses is observed. The beam is found to appear only when the plasma density scale length is small. Numerical simulations reveal that the electron beam is formed due to the confinement of the surface quasistatic electromagnetic fields. The results are of interest for potential applications of fast electron beams and deep understanding of the cone-target physics in the fast ignition related experiments.

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Cited by 169 publications
(105 citation statements)
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“…Electron beams with energies from tens to hundreds of kiloelectron-volts find wide application in various fields of science and technology (Mesyats, 2005;Li et al, 2006;Verbeeck et al, 2010). One of the most important parameters of electron beams is their energy spectrum.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…Electron beams with energies from tens to hundreds of kiloelectron-volts find wide application in various fields of science and technology (Mesyats, 2005;Li et al, 2006;Verbeeck et al, 2010). One of the most important parameters of electron beams is their energy spectrum.…”
Section: Introductionmentioning
confidence: 99%
“…Moreover, electrons of energy > eU m , where e is the electron charge and U m is the maximum gap voltage, are detected downstream of the anode foil of vacuum diodes at subnanosecond and nanosecond voltage pulse rise times (Khudyakova et al, 1964). The spectra of electron beams are measured with magnetic spectrometers (Bugaev et al, 1974;Mangles et al, 2004;Li et al, 2006) and time-of-flight spectrometers (Gloeckler & Hsieh, 1979). The spectra of nano-and subnanosecond electron beams are also measured with the use of different methods (Bugaev et al, 1974;Afanasiev et al, 2005;Baksht et al, 2007), including the measurements of beam current attenuation in foils of different thickness (Baksht et al, 2010).…”
Section: Introductionmentioning
confidence: 99%
“…This is different from the acceleration regime in previous works. 20,22,29,[42][43][44] The relativistic electrons can stay in phase with the co-moving laser electric field and be continuously accelerated for a long time until the laser pulse is reflected by the backside foil target.…”
Section: mentioning
confidence: 99%
“…A strong negative azimuthal magnetic field B x , of the order of a few hundred megagauss, is created and it tends to confine the electrons. Since the hot electrons have speeds close to that of light, balance of the electric (eE y ) and magnetic (ev e B x =c) forces tends to confine and collimate the electrons, so that the latter can propagate stably along the grated surface [16].…”
mentioning
confidence: 99%