“…Before we continue, we briefly mention that the timedependent nuclear wave functions can be expanded in a set of time-independent eigenfunctions, 9), applying the weak field approximation, which forbids the back transfer of population from the decaying state to the initial state, assuming a broad-band (vertical) excitation, using the local approximation, and introducing dressed states to remove the photoelectron energy E k 0 [60], brings the time-dependent Schrödinger equation for the total wave function, Eq. ( 9), into a set of coupled differential equations for the nuclear wave functions evolving on the decaying and final state, respectively,…”