Abstract

1. Introduction One of the most studied short-pulse laser-driven particle acceleration schemes is proton generation via the target-normal sheath-acceleration[1] mechanism, where hundreds of experiments[2] have been performed at facilities worldwide. This acceleration mechanism relies on the production of MeV energy electrons from the laser interaction with the target in order to produce 10’s of MeV proton energies. To date, most short-pulse experiments have been performed with single Gaussian-like pulses that are often not well characterized in terms of pulse-length and time-dependent intensity. This is in contrast to nanosecond-scale laser pulses that utilize pulse shaping technique to deliver precise pulse shapes for manipulating time-dependent physics. Such pulse shaping has allowed access to novel physics such as in Inertial Confinement Fusion (ICF) [3] and Equation of State (EOS) [4] experiments. It has similarly allowed for increased efficiency of laser-driven x-ray [5] and particle (proton or neutron) sources [6]. Multiple methods for generating custom pulse shapes at the sub-picosecond level already exist but are rarely employed for high-intensity laser-driven experiments. These methods include combining separate short-pulse beams, splitting and recombining single pulses, interferometric methods [7], or spectral shaping [8]. A limited number of experiments with some form of pulse shaping for high-intensity lasers have shown significant spectral enhancements to secondary sources such as MeV proton beams[9], implying that controlled manipulation of time-dependent particle acceleration physics is possible at the fs to ps level.

© 2020 The Author(s)