“…The important strong-field QED processes in lasercreated QED plasmas are [2,7,8]: (i) incoherent emission of > ∼ MeV energy gamma-ray photons by electrons and positrons on acceleration by the macroscopic electromagnetic fields in the laser-produced plasma (strongly nonlinear Compton scattering), with the resulting radiationreaction strongly modifying the dynamics of the emitting electron or positron [9,10]; (ii) pair creation by the emitted gamma-ray photons, in the same electromagnetic fields (the multi-photon Breit-Wheeler process [11]). For example: non-linear Compton scattering and the resulting radiation can lead to almost complete laser absorption [12,13]; pair cascades (where pairs emit further gamma-ray photons, which generate even more pairs), can lead to the creation of critical density pair plasmas [14][15][16][17]. It is therefore essential that we correctly include these QED processes in our models of the interaction of next-generation laser pulses with matter.…”