Optically controlled laser–plasma electron accelerator for compact gamma-ray sources

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 10 ^16 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 ( n _0 ∼ 10 ^19 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 10 ^6 photons within a microsteradian-scale observation cone.

Keywords

• laser wakefield accelerator
• blowout
• optical control of injection
• comb-like electron beams
• pulse stacking
• negative chirp