1992
DOI: 10.1017/s0263034600004237
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Scaling model for high-aspect-ratio microballoon direct-drive implosions at short laser wavelengths

Abstract: A scaling model for hot spherical ablative implosions in direct-drive mode is presented. The model results have been compared with experiments from LLE, ILE, and LLNL. Reduction of the neutron yield due to illumination nonuniformities is taken into account by the assumption that the neutron emission is cut off when the gas shock wave reflected off the center meets the incoming pusher, i.e., at a time when the probability of shell breakup is greatly enhanced. The main advantage of this semiempirical scaling mod… Show more

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Cited by 3 publications
(4 citation statements)
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“…If we assume 1-D fuel-pusher assembly, without mixing, from mass conservation, continuity of pressure, and temperature at the D-T-glass interface, the fuel compression is given by (Storm et al 1980) M DT and M p are, respectively, the fuel and pusher masses, (pAR) the pusher areal density, p m and pj the fuel densities, the index / corresponds to initial condition and m to the measured value at the burn time, Z p is the average pusher ionization, and a is approximate to 2. It can also be more simply evaluated from the pusher areal density by using a simple model.…”
Section: Results In Indirect-drive Schemementioning
confidence: 99%
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“…If we assume 1-D fuel-pusher assembly, without mixing, from mass conservation, continuity of pressure, and temperature at the D-T-glass interface, the fuel compression is given by (Storm et al 1980) M DT and M p are, respectively, the fuel and pusher masses, (pAR) the pusher areal density, p m and pj the fuel densities, the index / corresponds to initial condition and m to the measured value at the burn time, Z p is the average pusher ionization, and a is approximate to 2. It can also be more simply evaluated from the pusher areal density by using a simple model.…”
Section: Results In Indirect-drive Schemementioning
confidence: 99%
“…Numerous elements have been examined to be a tracer candidate to measure the areal density of either the fuel or the pusher (Campbell 1977;Lane 1980). The most commonly used for the pusher is 28 Si, but also used are Pr oxide by ILE (Miyanaga et al 1986) and at the present time Rb by LLNL (Lane et al 1990) on the powerful NOVA laser facility.…”
Section: Pusher Areal Density (Par) Measurementsmentioning
confidence: 99%
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