Abstract
We discuss the development of a new generation of accelerator-based hard X-ray sources driven exclusively by laser light. High-intensity laser pulses serve the dual roles: first, accelerating electrons by laser-driven plasma wakefields, and second, generating X-rays by inverse Compton scattering. Such all-laser-driven X-rays have recently been demonstrated to be energetic, tunable, relatively narrow in bandwidth, short pulsed and well collimated. Such characteristics, especially from a compact source, are highly advantageous for numerous advanced X-ray applications – in metrology, biomedicine, materials, ultrafast phenomena, radiology and fundamental physics.
Disclosure statement
No potential conflict of interest was reported by the author.
Notes
1. A light pulse propagates in plasma at the group velocity, , where ωp is the plasma frequency, defined by
, and ne is the plasma density. In highly under-dense plasmas, vg ∼ c, since in this case
, or ne
nc, where nc is the critical density, the density at which
.
2. When relativistic electrons, with v ≈ c, are accelerated, their kinetic energy increases much more rapidly than does their velocity, since the relativistic kinetic energy is ≈ γm0c2.
3. Photon energy spectral densities, or photon energy per unit bandwidth (MeV/MeV), can be peaked due to the nonuniform photon energy weighting. However, the same spectrum may not be peaked when plotted as photon number spectral density, photon number per unit bandwidth (MeV−1), which has even energy weighting.