Abstract

We report on the first observation of tertiary reaction-in-flight (RIF) neutrons produced in compressed deuterium and tritium filled capsules using the National Ignition Facility at Lawrence Livermore National Laboratory, Livermore, CA. RIF neutrons are produced by third-order, out of equilibrium (“in-flight”) fusion reactions, initiated by primary fusion products. The rate of RIF reactions is dependent upon the range of the elastically scattered fuel ions and therefore a diagnostic of Coulomb physics within the plasma. At plasma temperatures of ∼5 keV, the presence of neutrons with kinetic energies greater than 15 MeV is a unique signature for RIF neutron production. The reaction <sup>169</sup>Tm(n,3n)<sup>167</sup>Tm has a threshold of 15.0 MeV, and a unique decay scheme making it a suitable diagnostic for observing RIF neutrons. RIF neutron production is quantified by the ratio of <sup>167</sup>Tm/<sup>168</sup>Tm observed in a <sup>169</sup>Tm foil, where the reaction <sup>169</sup>Tm(n,2n)<sup>168</sup>Tm samples the primary neutron fluence. Averaged over 4 implosions1<sup>–4</sup> at the NIF, the <sup>167</sup>Tm/<sup>168</sup>Tm ratio is measured to be 1.5 &plusmn; 0.3 x 10<sup>−5</sup>, leading to an average ratio of RIF to primary neutron ratio of 1.0 &plusmn; 0.2 x 10<sup>−4</sup>. These ratios are consistent with the predictions for charged particle stopping in a quantum degenerate plasma.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.