Abstract

We address the problem of energy dispersion of radiation pressure accelerated (RPA) ion beams emerging from a thin target. Two different acceleration regimes, namely phase-stable acceleration and multistage acceleration, are considered by means of analytical modeling and one-dimensional particle-in-cell simulations. Our investigations offer a deeper understanding of RPA and allow us to derive some guidelines for generating monoenergetic ion beams.

Highlights

  • Interaction of ultra-intense laser pulses with thin foils offers interesting possibilities to generate energetic charged particles

  • In contrast to target normal sheath acceleration (TNSA) [1, 2], where ions are accelerated from the target rear surface in the electrostatic field built up by the laser-created hot electrons, radiation pressure acceleration (RPA) of ion beams relies on the efficient momentum transfer from laser photons to ions in a thin dense target, which reflects the incident laser pulse

  • The description proposed here allows for a greater insight in the details of RPA of thin foils than that available from the standard macroscopic light-sail model

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Summary

Introduction

Interaction of ultra-intense laser pulses with thin foils offers interesting possibilities to generate energetic charged particles. We first recall the basic modelling of RPA of a thin foil and provide scaling laws concerning the maximum ion energy that can be reached as a function of the laser intensity or power (Sec. 2). Beyond this simple (macroscopic) modelling, we discuss the details of RPA of a thin foil as following from two complementary processes.

Basic Modelling
Macroscopic approach: the light-sail model
Scaling laws for the ion energy
Two RPA regimes
Phase-stable acceleration of thin targets
Multi-stage RPA of thicker targets
Numerical simulations
Optimal target thickness
Ion acceleration in the phase-stable regime
Ion acceleration in the multi-stage regime
Findings
Conclusion
Full Text
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