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Experimental results of radiation-driven, layered deuterium-tritium implosions with adiabat-shaped drives at the National Ignition Facility
Radiation-driven, layered deuterium-tritium (DT) implosions were carried out using 3-shock and 4-shock “adiabat-shaped” drives and plastic ablators on the National Ignition Facility (NIF) [E. M. Campbell et al., AIP Conf. Proc. 429, 3 (1998)]. The purpose of these shots was to gain further understan...
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Published in: | Physics of plasmas 2016-10, Vol.23 (10) |
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Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
Format: | Article |
Language: | English |
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Summary: | Radiation-driven, layered deuterium-tritium (DT) implosions were carried out using
3-shock and 4-shock “adiabat-shaped” drives and plastic ablators on the National Ignition
Facility (NIF) [E. M. Campbell et al., AIP Conf. Proc.
429, 3 (1998)]. The purpose of these shots was to gain further
understanding on the relative performance of the low-foot implosions of the National
Ignition Campaign [M. J. Edwards et al., Phys. Plasmas
20, 070501 (2013)] versus the subsequent high-foot implosions [T. Döppner
et al., Phys. Rev. Lett. 115, 055001 (2015)].
The neutron yield
performance in the experiment with the 4-shock adiabat-shaped drive was improved by
factors ∼3 to ∼10, compared to five companion low-foot shots despite large low-mode
asymmetries of DT fuel, while measured compression was similar to its low-foot companions.
This indicated that the dominant degradation source for low-foot implosions was
ablation-front instability growth, since adiabat shaping significantly stabilized this
growth. For the experiment with the low-power 3-shock adiabat-shaped drive, the DT fuel
compression was significantly increased, by ∼25% to ∼36%, compared to its companion
high-foot implosions. The neutron yield increased by ∼20%, lower than the increase of ∼50%
estimated from one-dimensional scaling, suggesting the importance of residual
instabilities
and asymmetries. For the experiment with the high-power, 3-shock adiabat-shaped drive, the
DT fuel compression was slightly increased by ∼14% compared to its companion high-foot
experiments. However, the compression was reduced compared to the lower-power 3-shock
adiabat-shaped drive, correlated with the increase of hot electrons that hypothetically
can be responsible for reduced compression in high-power adiabat-shaped experiments as
well as in high-foot experiments. The total neutron yield in the high-power 3-shock adiabat-shaped shot
N150416 was 8.5 × 1015 ± 0.2 × 1015, with the fuel areal density of
0.90 ± 0.07 g/cm2, corresponding to the ignition threshold factor parameter
IFTX (calculated without alpha heating) of 0.34 ± 0.03 and the yield amplification due to
the alpha heating of 2.4 ± 0.2. The performance parameters were among the highest of all
shots on NIF and the closest to ignition at this time, based on the IFTX metric. The
follow-up experiments were proposed to continue testing physics hypotheses, to measure
implosion reproducibility, and to improve quantitative understanding on present implosion
results. |
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ISSN: | 1070-664X 1089-7674 |
DOI: | 10.1063/1.4964919 |