“…In the nonlinear laser-driven bubble regime, where the particles are self-trapped, simulations and experiments show that an electron beam with σ x ∼ 0.1 µm, σ px /(m e c) ∼ 1, and n ∼ 0.1 mm mrad can be achieved [3], where σ x is the root-mean-square (rms) beam radius, σ px /(m e c) is the normalized rms transverse momentum, and the normalized transverse emittance can be estimated as n σ x σ px /(m e c). High-quality, laserplasma-accelerated electron beams could be good candidates to drive free-electron lasers, enabling a new generation of low-cost, compact light sources [4,5]. Improved beam phase space characteristics, and, in particular, reduced transverse emittance, is highly desired for light sources and other applications.…”