1978
DOI: 10.1103/physrevlett.40.42
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Properties of Resonantly Heated Electron Distributions

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Cited by 295 publications
(124 citation statements)
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“…In the case of a p-polarized laser beam, it is well known that in experimental conditions similar to ours, the hot electrons could be generated by two mechanisms -resonance absorption (RA) and vacuum heating (VH). RA has been well studied both experimentally [17,18,19,20] and theoretically [21,22,23,24] and based on the observations and simulations, the following scaling law [21] has been established:…”
mentioning
confidence: 99%
“…In the case of a p-polarized laser beam, it is well known that in experimental conditions similar to ours, the hot electrons could be generated by two mechanisms -resonance absorption (RA) and vacuum heating (VH). RA has been well studied both experimentally [17,18,19,20] and theoretically [21,22,23,24] and based on the observations and simulations, the following scaling law [21] has been established:…”
mentioning
confidence: 99%
“…Thus we argue that the electrostatic plasma waves generated by the RA mechanism (typically with E 2 /4πn e T e ≫ 1 ) during the laser pulse will continue to slowly damp (or convect away) and accelerate electrons for a few hundred femtoseconds after the laser pulse. To get an estimate of S 0 , which is the magnitude of the source term | (c/σ)( ∇ × j hot ) | , we evaluate j hot ≈ f a eI/T hot by taking a conversion fraction (f a ) of incident energy into hot electrons as 0.3 and T hot ∼ 20 keV (estimated by using the well known scaling laws for resonance absorption [21]). This yields hot electron current density j hot ∼ 4.5 × 10 20 statampere/cm 2 .…”
mentioning
confidence: 99%
“…4,23,24,34 The tantalum target ͑atomic number Z͒ is subjected to the assumed electron energy distribution, f (E e ) ͓1/keV͔, and generates a bremsstrahlung distribution, g(E B ), which is modelled according to the expression 35,36 g͑E B ͒Ϸ2ϫ10…”
Section: Theorymentioning
confidence: 99%
“…The mirror reflects the light back at 60°t o the incoming beam, giving an angle of incidence of 30°at the target; close to the optimum. 23,[25][26][27] The converging light passes through a 110-m-thick glass plate ͑optical microscopy cover plate͒ and focuses onto the solid target. The parabolic mirror is aligned in air by gradually lowering the laser pulse energy while adjusting the mirror mount and maintaining a visible spark in the focus.…”
Section: The X-ray Generation Setupmentioning
confidence: 99%
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