“…A further and most useful approximation is the target Kohn-Sham approximation [12], which consists in substituting Dyson orbitals by the relevant Kohn-Sham orbitals, along with ad hoc or calculated spectroscopic pole strengths, in order to account for the flux of ionization intensity toward shake-up [13] and valence correlation bands [14] at higher electron binding energies. In many cases, (rescaled) Kohn-Sham orbitals are empirically known to be excellent approximations to Dyson orbitals [15,16]. In practice, however, the interpretation of EMS experiments is subject to numerous complications such as: overlap effects in overcrowed ionization bands [17,18], conformational mobility [19][20][21] and (thermally induced) nuclear dynamics in the electronic initial (neutral) ground state [22], shake-up processes due to electronic configuration interactions in the final ionized state [23][24][25][26], distorted wave and post-collision (e.g., rescattering) effects [27][28][29][30][31][32][33], and possibly ultra-fast nuclear dynamics in the final ionized state, in the form of bond breaking [22] or Coulomb explosion processes [34][35][36], as well as Jahn-Teller distortions [37] in the final ionized state.…”