“…For laser-driven wakefield accelerators (LWFAs), energies up to 8 GeV energy gain have been reported [ 7 ] , as well as per-mille level energy spread [ 8 ] , 10–100 pC charge, few-femtosecond beam duration [ 9 ] , sub-millirad divergence, few-micrometer source size [ 10 ] , and repetition rates up to 10 Hz (and planned for kilohertz). For beam-driven wakefield accelerators (PWFAs), energies up to 84 GeV (42 GeV energy gain) have been reported [ 11 ] , as well as per-mille-level energy spread [ 12 , 13 ] , 10–100 pC charge, tens of femtosecond beam duration [ 14 , 15 ] , micrometer-level normalized emittance [ 16 ] , 10 m level source size, and few hertz repetition rates. With these properties already having been demonstrated, there are a growing number of experimental programs interested in using these electron beams to drive next-generation light sources.…”