Sensitivity of the dynamic-shell target to laser drive nonuniformities

The dynamic-shell concept for inertial confinement fusion (ICF) uses an initially homogeneous target and a carefully shaped laser pulse to form a shell and implode it. The laser pulse consists of a series of pickets that drive shocks into the target. The first few shocks converge inwards and rebound from the center of the target, creating an expanding, low-density plasma. Subsequent shocks are launched into the expanding plasma and eventually coalesce to form a shell, which is then imploded with a traditional ICF laser pulse. This study describes radiation-hydrodynamic simulations that investigate the sensitivity of dynamic-shell targets to imperfections in the laser drive. A one-dimensional (1D) study looks at mistiming and power variations in the pickets and a two-dimensional (2D) study examines irradiation perturbations imposed by the laser-beam geometry. Simulations show that less than ∼2% power imbalance or 200 ps timing variation in the pickets is sufficient to keep the yield above 90% of the maximum. Additionally, the 2D simulations show that 72 or more beams are required to keep irradiation nonuniformities low enough to obtain fusion yields close to that of 1D simulations.

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Publication Details

Journal
Physical review. E
Published
2025-02-28
DOI
https://doi.org/10.1103/physreve.111.025210
Citations
1
Primary Topic
Laser-Plasma Interactions and Diagnostics
Type
article
Field-Weighted Citation Impact
1.87

Funders

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article

Sensitivity of the dynamic-shell target to laser drive nonuniformities

V. N. Goncharov, A. Shvydky, T. J. B. Collins, I. V. Igumenshchev et al.
1 citations
Physical review. E
Laser-Plasma Interactions and Diagnostics
1.87
article

Sensitivity of the dynamic-shell target to laser drive nonuniformities

V. N. Goncharov, A. Shvydky, T. J. B. Collins, I. V. Igumenshchev, William Trickey
article en
1 citations

Abstract

The dynamic-shell concept for inertial confinement fusion (ICF) uses an initially homogeneous target and a carefully shaped laser pulse to form a shell and implode it. The laser pulse consists of a series of pickets that drive shocks into the target. The first few shocks converge inwards and rebound from the center of the target, creating an expanding, low-density plasma. Subsequent shocks are launched into the expanding plasma and eventually coalesce to form a shell, which is then imploded with a traditional ICF laser pulse. This study describes radiation-hydrodynamic simulations that investigate the sensitivity of dynamic-shell targets to imperfections in the laser drive. A one-dimensional (1D) study looks at mistiming and power variations in the pickets and a two-dimensional (2D) study examines irradiation perturbations imposed by the laser-beam geometry. Simulations show that less than ∼2% power imbalance or 200 ps timing variation in the pickets is sufficient to keep the yield above 90% of the maximum. Additionally, the 2D simulations show that 72 or more beams are required to keep irradiation nonuniformities low enough to obtain fusion yields close to that of 1D simulations.

Physical review. EVol. 111(2)
Energetics (United States) (US), University of Rochester (US)
U.S. Department of Energy, University of Rochester, National Nuclear Security Administration
Openalex Percentile: Top 15%
Laser-Plasma Interactions and Diagnostics
1.87
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Sensitivity of the dynamic-shell target to laser drive nonuniformities — V. N. Goncharov, A. Shvydky, et al. · Physical review. E (2025) | TGRS Research Map | TGRS