2017
DOI: 10.1103/physrevlett.118.205001
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Collimated Propagation of Fast Electron Beams Accelerated by High-Contrast Laser Pulses in Highly Resistive Shocked Carbon

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Cited by 12 publications
(9 citation statements)
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“…Note that the density range is from 1 to -10 g cm 3 and the temperatures from 1 to 10 eV indicating the WDM initial conditions of the transport target. The background electron temperature upon injecting the REB remains below 100 eV for~ps, specifically at the edges of the REB where the resistive gradient field is developing, further justifying the importance of carefully computing the resistivity in WDM for accurate prediction of the REB transport [49,54]. Further details on the hydrodynamic modeling are given in the Methods section.…”
Section: Resultsmentioning
confidence: 99%
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“…Note that the density range is from 1 to -10 g cm 3 and the temperatures from 1 to 10 eV indicating the WDM initial conditions of the transport target. The background electron temperature upon injecting the REB remains below 100 eV for~ps, specifically at the edges of the REB where the resistive gradient field is developing, further justifying the importance of carefully computing the resistivity in WDM for accurate prediction of the REB transport [49,54]. Further details on the hydrodynamic modeling are given in the Methods section.…”
Section: Resultsmentioning
confidence: 99%
“…When comparing the hot electron density and background electron temperature for undriven VC (figures 6(a)-(b)) and for driven VC at D = t 20.5 ns (figures 6(c)-(d)) at early time ( = t 1 ps), we can already notice a significant difference in the REB transport for the two cases. The temperature gradients at the edges of the beam are the location of the strong resistive B-field (see next in figure 7) that will impact the beam propagation [49,54]. Next, we show how it eventually affects the beam at later time (4 ps).…”
Section: Relativistic Electron Transport Modelingmentioning
confidence: 91%
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“…Different strategies to control REB propagation in solid matter have been proposed. They rely on the use of ~kT magnetic fields, which can be externally generated by coils 27,28 or self generated 29 , either by artificial resistivity gradients 3034 or by exploiting the intrinsically high resistivity of a material 35 . One of the schemes by using self-generated magnetic fields was proposed by A. Robinson et al .…”
Section: Introductionmentioning
confidence: 99%
“…Different strategies to control REB propagation in solid matter have been proposed. They rely on the use of ∼kT magnetic fields, which can be externally generated by coils [184,10] or self generated [20], either by artificial resistivity gradients [110,191,53,185,164] or by exploiting the intrinsically high resistivity of a material [211].…”
Section: Electron Beam Collimation Schemesmentioning
confidence: 99%