“…, the distribution of binding energies along the classical MD trajectory:
where ρ ( R[combining right harpoon above] ) is the nuclear density evaluated with the classical MD simulations, BE n is the binding energy of the ejected electron, KE is the kinetic energy of an ejected electron, E is the incident photon energy, and f Fr, n is the contribution from the n -th electron of the fragment of interest. In the modelled photoemission spectra we included solvent spectral broadening via the reflection principle with an additional broadening scheme (RP-AB),89 i.e. , each point is broadened with a Gaussian function with a variance reflecting the reorganization energy calculated by means of dielectric continuum methods.…”