2006
DOI: 10.1103/physreve.73.016402
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Stopping, straggling, and blooming of directed energetic electrons in hydrogenic and arbitrary-Zplasmas

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Cited by 23 publications
(18 citation statements)
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“…8,9 To illustrate this, we consider a 1-MeV electron beam (beam radius r b =10 µm) in a compressed DT target (ρ=300 g/cm 3 and T e =5 keV). The maximum field B max = µ 0 I b /(2πr b ) occurs at the beam surface, where…”
Section: Corementioning
confidence: 99%
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“…8,9 To illustrate this, we consider a 1-MeV electron beam (beam radius r b =10 µm) in a compressed DT target (ρ=300 g/cm 3 and T e =5 keV). The maximum field B max = µ 0 I b /(2πr b ) occurs at the beam surface, where…”
Section: Corementioning
confidence: 99%
“…Thus a criterion for distinguishing the interaction regimes and for illustrating their relative importance 9 is approximately established based on above physics arguments as …”
Section: Corementioning
confidence: 99%
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“…It has great potential advantages over conventional ICF, notably in relaxing the requirements of implosion symmetry and hydrodynamic instabilities, leading to higher gains with lower driver energy, which has drawn significant attention worldwide [2][3][4][5][6][7][8][9]. In FI scheme, fast electrons generated via ultraintense (∼10 20 W/cm 2 ) short-pulse (∼ 20 ps) laser interaction with plasmas will transport into the pre-compressed dense core to deposit energy locally, forming the hot spot.…”
Section: Introductionmentioning
confidence: 99%