“…In metals, as already briefly explained in the introduction, the laser pulse is absorbed by an abundance of free electrons. In dielectric materials, nonlinear processes such as multi-photon ionization lead to the transition of electrons from the valence to the conduction band, which enables the direct interaction of the laser with the generated free charge carriers in the conduction band [41,42]. Various modelling approaches for the rate of the generation of free charge carriers by strong electric field ionization (SFI) are based on the so-called Keldysh theory, which calculates an ionization rate depending on the band gap and the reduced effective mass of the electron-hole pairs [42,43].…”