Use of 41Ar production to measure ablator areal density in NIF beryllium implosions

For the first time, 41Ar produced by the (n,ϒ) reaction from 40Ar in the beryllium shell of a DT filled Inertial Confinement Fusion capsule has been measured. Ar is co-deposited with beryllium in the sputter deposition of the capsule shell. Combined with a measurement of the neutron yield, the radio...

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Veröffentlicht in:Physics of plasmas 2017-02, Vol.24 (2)
Hauptverfasser: Wilson, D. C., Cassata, W. S., Sepke, S. M., Velsko, C. A., Huang, H., Yeamans, C. B., Kline, J. L., Yi, A., Simakov, A. N., Haan, S. W., Batha, S. H., Dewald, E. L., Rygg, J. R., Tommasini, R., Xu, H., Kong, C., Bae, J., Rice, N.
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Sprache:eng
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Zusammenfassung:For the first time, 41Ar produced by the (n,ϒ) reaction from 40Ar in the beryllium shell of a DT filled Inertial Confinement Fusion capsule has been measured. Ar is co-deposited with beryllium in the sputter deposition of the capsule shell. Combined with a measurement of the neutron yield, the radioactive 41Ar then quantifies the areal density of beryllium during the DT neutron production. The measured 1.15 ± 0.17 × 10+8 atoms of 41Ar are 2.5 times that from the best post-shot calculation, suggesting that the Ar and Be areal densities are correspondingly higher than those calculated. Possible explanations are that (1) the beryllium shell is compressed more than calculated, (2) beryllium has mixed into the cold DT ice, or more likely (3) less beryllium is ablated than calculated. Since only one DT filled beryllium capsule has been fielded at NIF, these results can be confirmed and expanded in the future.
ISSN:1070-664X
1089-7674
DOI:10.1063/1.4975187