2015
DOI: 10.1063/1.4905669
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Refluxed electrons direct laser acceleration in ultrahigh laser and relativistic critical density plasma interaction

Abstract: We analyze the motion of the plasma critical layer by two different processes in the relativistic-electron laser-plasma interaction regime ða 0 > 1Þ. The differences are highlighted when the critical layer ions are stationary in contrast to when they move with it. Controlling the speed of the plasma critical layer in this regime is essential for creating low-b traveling acceleration structures of sufficient laser-excited potential for laser ion accelerators. In Relativistically Induced Transparency Acceleratio… Show more

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Cited by 2 publications
(2 citation statements)
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“…Figure 3(a) illustrates the hot electron spectrum for different chirp parameters at 60 T. It is obvious that the electron distribution for negative chirped pulse is unfavorable. The slope of the electron distribution is representative of the effective temperature [24]. As the dashed lines show, the slope of the line related to the positive chirped pulse is higher than that one for unchirped pulse.…”
Section: Chirp Effectmentioning
confidence: 96%
See 1 more Smart Citation
“…Figure 3(a) illustrates the hot electron spectrum for different chirp parameters at 60 T. It is obvious that the electron distribution for negative chirped pulse is unfavorable. The slope of the electron distribution is representative of the effective temperature [24]. As the dashed lines show, the slope of the line related to the positive chirped pulse is higher than that one for unchirped pulse.…”
Section: Chirp Effectmentioning
confidence: 96%
“…In order to directly accelerate the protons or ions by laser, the laser intensity in order of 10 W cm 24 2…”
Section: > -mentioning
confidence: 99%