1985
DOI: 10.1088/0029-5515/25/9/067
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Light-ion beams for inertial confinement fusion

Abstract: Inertial confinement fusion requires the generation and focusing of several megajoules of energy at > 100 TW power and >100 TWcm" 2 power density onto a target for approximately 10 ns. Lasers and particle beam drivers have been developed for this purpose. Light-ion beams offer the potential for a costeffective, efficient and versatile driver with excellent energy deposition and no significant preheat. The research and development to date has emphasized technology development of the driver. Advances in pulsed p… Show more

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Cited by 3 publications
(2 citation statements)
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“…An intense-ion beam (IIB) is a plasma beam with far greater particle energy and instantaneous intensity, with typical output parameters, W i ≃100-1000's of keV ion energy, n i ≲ 10 17 − 10 19 m −3 ion density, τ b ≃ 0.1 − 1 µs pulse-duration, and Pb ≃ 10 9 − 10 12 W instantaneous-peak power. IIBs were originally developed in the late 70's for light-ion, inertialconfinement fusion [9,10] and later adapted for use in fieldreversed fusion plasmas [11,12] and materials processing [13,14]. Early designs used flashover discharges to produce a high-density plasma from which the ions were extracted and then accelerated.…”
Section: Introductionmentioning
confidence: 99%
“…An intense-ion beam (IIB) is a plasma beam with far greater particle energy and instantaneous intensity, with typical output parameters, W i ≃100-1000's of keV ion energy, n i ≲ 10 17 − 10 19 m −3 ion density, τ b ≃ 0.1 − 1 µs pulse-duration, and Pb ≃ 10 9 − 10 12 W instantaneous-peak power. IIBs were originally developed in the late 70's for light-ion, inertialconfinement fusion [9,10] and later adapted for use in fieldreversed fusion plasmas [11,12] and materials processing [13,14]. Early designs used flashover discharges to produce a high-density plasma from which the ions were extracted and then accelerated.…”
Section: Introductionmentioning
confidence: 99%
“…There is a growing theoretical literature on the macroscopic (Davidson, Tsang & Swegle 1984a;Swegle 1983;Swegle & Ott 1981a, b;Davidson & Tsang 1984, 1985Chang et al 1984;Chernin & Lau 1984;Davidson, Tsang & Uhm 1985) and kinetic (Davidson 1985a, b; equilibrium and stability properties of intense non-neutral electron flow, with applications that range from high-voltage diodes for particle-beam fusion (VanDevender et al 1981, 1985 andreferences therein;Miller 1982) to coherent radiation generation by relativistic magnetrons (Orzechowski & Bekefi 1979;Palevsky & Bekefi 1979;Bekefi 1982;Davidson, McMullin & Tsang 19846;. In the present analysis, we make use of the extraordinary-mode eigenvalue equation derived in Davidson et al (1984) for general equilibrium profiles to investigate the local stability properties (Krall 1968) of relativistic, non-neutral electron flow in the planar diode configuration illustrated in figure 1.…”
Section: Introductionmentioning
confidence: 99%