Decreasing Necessary Optimization Time For Increases In Neutron Yieldof Direct-Drive Inertial Confinement Fusion ImplosionsUsing a Three-Dimensional Contoured Fuel Shell
POSTER
Abstract
In the pursuit of achieving energy output exceeding input in direct-drive inertial
confinement fusion, ensuring uniform fuel compression in the final implosion
stages presents a significant challenge. In experimental setups, energy is delivered using a
finite number of beams spaced in a spherical geometry (e.g., 60 beams for OMEGA 1 ) and
results in uneven laser-energy deposition, with some regions becoming hotter than
others. Consequently, the compression becomes aspherical, leading to a
perturbed implosion during the critical stage of maximum fusion reactions (i.e., “bang
time”;). By employing the 3-D code ASTER2, our objective in
this simulation is to enhance the neutron yield by adjusting the thickness of the target
shell in three dimensions, in order to account for the spherical asymmetry present at bang
time. To assess the effectiveness of this approach, we calculate the sphericity of the target
at various time points, including bang time. As the sphericity approaches unity, it should
correlate with increasing neutron yields. This is even true for time points preceding bang
-time, therefore eliminating the need to simulate implosions until bang time and
also saving valuable optimization time.
confinement fusion, ensuring uniform fuel compression in the final implosion
stages presents a significant challenge. In experimental setups, energy is delivered using a
finite number of beams spaced in a spherical geometry (e.g., 60 beams for OMEGA 1 ) and
results in uneven laser-energy deposition, with some regions becoming hotter than
others. Consequently, the compression becomes aspherical, leading to a
perturbed implosion during the critical stage of maximum fusion reactions (i.e., “bang
time”;). By employing the 3-D code ASTER2, our objective in
this simulation is to enhance the neutron yield by adjusting the thickness of the target
shell in three dimensions, in order to account for the spherical asymmetry present at bang
time. To assess the effectiveness of this approach, we calculate the sphericity of the target
at various time points, including bang time. As the sphericity approaches unity, it should
correlate with increasing neutron yields. This is even true for time points preceding bang
-time, therefore eliminating the need to simulate implosions until bang time and
also saving valuable optimization time.
Publication: 1 T. R. Boehly et al., Opt. Commun. 133, 495 (1997).<br>2 I. V. Igumenshchev et al., Phys. Plasmas 23, 052702 (2016).
Presenters
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Justin Florence
Laser Laboratory of Energetics
Authors
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Justin Florence
Laser Laboratory of Energetics