Abstract
Recent advances in Inertial Confinement Fusion (ICF) experiments at Lawrence Livermore National Laboratory's National Ignition Facility (NIF) have underscored the need for accurate total yield measurements of DT neutrons because yield measurements provide a measure of the predicted performance of the experiments. Future gas-puff DT experiments at Sandia National Laboratory's Z facility will also require similar measurements. For ICF DT experiments, the standard technique for measuring the neutron (14.1MeV) yield, counts the activity (counts/minute) induced in irradiated copper samples. This activity occurs by the 63 Cu(n,2n) 62 Cu reaction where 62 Cu decays by positrons ( +) with a half-life of 9.67 minutes. The calibrations discussed here employ the associated-particle method (APM), where the ( 4 He) particles from the T(d,n) 4 He reaction are measured to infer neutron fluxes on a copper sample. The flux induces 62 Cu activity, measured in a coincidence counting system. The method leads to a relationship between a DT neutron yield and copper activity known as the F-factor. The goal in future experiments is to apply this calibration to measure the yield at NIF with a combined uncertainty approaching 5%.
Highlights
Recent advances in Inertial Confinement Fusion (ICF) experiments at Lawrence Livermore National Laboratory’s National Ignition Facility (NIF) have underscored the need for accurate total yield measurements of DT neutrons because yield measurements provide a measure of the predicted performance of the experiments
We have developed a Lawrence Livermore’s National Ignition Facility (NIF) DT neutron diagnostic (NAD20), based on the activation of copper via 63Cu(n, 2n)62Cu reaction with a half-life of 9.67 min. for 62Cu and a dedicated nuclear electronics counting system
We report here progress on a technique to calibrate the activation of copper and the counting system
Summary
We have developed a Lawrence Livermore’s National Ignition Facility (NIF) DT neutron diagnostic (NAD20), based on the activation of copper via 63Cu(n, 2n)62Cu reaction with a half-life of 9.67 min. for 62Cu and a dedicated nuclear electronics counting system. For ICF DT experiments, the standard technique for measuring the neutron (14.1 MeV) yield, counts the activity (counts/minute) induced in irradiated copper samples.
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