Abstract

Generating quasi-monochromatic, femtosecond γ-ray pulses via Thomson scattering (TS) demands exceptional electron beam (e-beam) quality, such as percent-scale energy spread and five-dimensional brightness over 1016 A m–2. We show that near-GeV e-beams with these metrics can be accelerated in a cavity of electron density, driven with an incoherent stack of Joule-scale laser pulses through a mm-size, dense plasma (n0 ∼ 1019 cm−3). Changing the time delay, frequency difference, and energy ratio of the stack components controls the e-beam phase space on the femtosecond scale, while the modest energy of the optical driver helps afford kHz-scale repetition rate at manageable average power. Blue-shifting one stack component by a considerable fraction of the carrier frequency makes the stack immune to self-compression. This, in turn, minimizes uncontrolled variation in the cavity shape, suppressing continuous injection of ambient plasma electrons, preserving a single, ultra-bright electron bunch. In addition, weak focusing of the trailing component of the stack induces periodic injection, generating, in a single shot, a train of bunches with controllable energy spacing and femtosecond synchronization. These designer e-beams, inaccessible to conventional acceleration methods, generate, via TS, gigawatt γ-ray pulses (or multi-color pulse trains) with the mean energy in the range of interest for nuclear photonics (4–16 MeV), containing over 106 photons within a microsteradian-scale observation cone.

Highlights

  • Inverse Compton scattering [1,2,3,4,5,6,7,8] is an emerging technique for obtaining quasi-monochromatic, strongly collimated γ-ray pulses through the collision of a short, quasi-monoenergetic electron beam (QME e-beam) and a near- to mid-IR interaction laser pulse (ILP)

  • Our simulations show that emulating a step-wise negative chirp, by advancing the higher-frequency component of the stack in time, nearly doubles electron energy compared to the predictions of the accepted scalings, demonstrating a near-GeV gain in a mm-scale, dense plasma (n0 ∼ 1019 cm−3) along with a boost in brightness to a few 1017 A m–2

  • In a conventional laser–plasma accelerator (LPA), electrons self-injected from the ambient plasma are accelerated in the plasma wake bucket—a cavity of electron density maintained by the radiation pressure of a single narrow-bandwidth laser pulse

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Summary

February 2018

Keywords: laser wakefield accelerator, blowout, optical control of injection, comb-like electron beams, pulse stacking, negative chirp, Original content from this inverse Compton/Thomson scattering work may be used under the terms of the Creative Commons Attribution 3.0 licence.

Introduction
Interaction regimes and simulation methods
Generating trains of e-bunches and comb-like γ-ray beams
Optically controlled quasi-monochromatic TS γ-ray pulses
Findings
Summary and outlook
Full Text
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