Abstract

The role of the coronal electron plasma temperature for shock-ignition conditions is analysed with respect to the dominant parametric processes: stimulated Brillouin scattering, stimulated Raman scattering, two-plasmon decay (TPD), Langmuir decay instability (LDI) and cavitation. TPD instability and cavitation are sensitive to the electron temperature. At the same time the reflectivity and high-energy electron production are strongly affected. For low plasma temperatures the LDI plays a dominant role in the TPD saturation. An understanding of laser–plasma interaction in the context of shock ignition is an important issue due to the localization of energy deposition by collective effects and hot electron production. This in turn can have consequences for the compression phase and the resulting gain factor of the implosion phase.

Highlights

  • The principal constituents of shock ignition (SI), converging shocks and their returns in spherical or cylindrical geometry, are based on ideas suggested some time ago[1,2,3], before it was applied for concrete applications in inertial confinement fusion (ICF)[4,5,6,7,8]

  • This paper considers in some detail the role of the coronal electron plasma temperature as far as the SI scenario is concerned

  • For the cold case c8, two-plasmon decay (TPD) is saturated by Langmuir decay instability (LDI) which develops on the EPWs generated originally by TPD

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Summary

Introduction

One of the important results of kinetic simulations of LPI in the framework of SI is the fact that the laser energy is absorbed not at the critical density via inverse Bremsstrahlung but by collective effects in the low-density plasma corona[19,20,21,22,23,24]. This affects the gain considerably as far as ignition is concerned[11].

Simulation setup
Characterization of the parametric instabilities involved
Overall scenario
Reflectivity
Electron-related mode activity
Plasma cavitation
Laser absorption into hot electrons
Conclusions
Full Text
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