Published in

American Institute of Physics, Physics of Plasmas, 8(29), p. 082704, 2022

DOI: 10.1063/5.0097080

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Role of hot electrons in shock ignition constrained by experiment at the National Ignition Facility

This paper was not found in any repository, but could be made available legally by the author.
This paper was not found in any repository, but could be made available legally by the author.

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Abstract

Shock ignition is a scheme for direct drive inertial confinement fusion that offers the potential for high gain with the current generation of laser facility; however, the benefits are thought to be dependent on the use of low adiabat implosions without laser–plasma instabilities reducing drive and generating hot electrons. A National Ignition Facility direct drive solid target experiment was used to calibrate a 3D Monte Carlo hot-electron model for 2D radiation-hydrodynamic simulations of a shock ignition implosion. The [Formula: see text] adiabat implosion was calculated to suffer a 35% peak areal density decrease when the hot electron population with temperature [Formula: see text] and energy [Formula: see text] was added to the simulation. Optimizing the pulse shape can recover [Formula: see text] of the peak areal density lost due to a change in shock timing. Despite the harmful impact of laser–plasma instabilities, the simulations indicate shock ignition as a viable method to improve performance and broaden the design space of near ignition high adiabat implosions.