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Hot-electron surface retention in intense short-pulse laser-matter interactions
R J Mason1, E S Dodd, B J Albright
1Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA. mason@lanl.gov
Summary
Implicit hybrid plasma simulations show hot electrons can be retained near target surfaces with steep density gradients. This energy retention, driven by magnetic fields and geometric effects, could aid fast ignition laser fusion.
Area of Science:
- Plasma physics
- Laser-plasma interactions
- Computational physics
Background:
- Intense short-pulse lasers deposit energy into hot electrons in plasma.
- Understanding hot electron behavior is crucial for applications like inertial confinement fusion.
- Steep density gradients and magnetic fields influence electron transport.
Purpose of the Study:
- To investigate the retention of hot electron energy near the surface of plasma targets.
- To explore the mechanisms behind hot electron confinement in laser-irradiated targets.
- To assess the implications of hot electron retention for applications such as fast ignition and radiography.
Main Methods:
- Implicit hybrid plasma simulations were employed.
- Analysis focused on targets with steep density gradients illuminated by intense short-pulse lasers.
- Mechanisms considered include lateral electron transport, spontaneous magnetic fields, geometric effects, and electric fields.
Main Results:
- A significant fraction of deposited energy is retained in hot electrons near the target surface.
- Hot electron retention is influenced by lateral transport, spontaneous magnetic fields, and ponderomotive force effects.
- Axial focusing of hot electrons into the target occurs due to magnetic fields.
- Filamentation of hot electrons can occur in moderate Z targets via resistive Weibel-like instability.
Conclusions:
- Engineered hot electron retention, combined with ponderomotive density profile steepening, may reduce hot electron range, benefiting fast ignition.
- Alternatively, uncontrolled retention could hinder deeper energy deposition required for radiography and fast ion generation.