“…Consequently, upon electronic excitation of E, an intramolecular electronic charge redistribution occurs in E* that leads to the formation of the keto (K*) or zwitterion (Z*) tautomer. When these species return to S 0 , they can be stabilized in this or other tautomeric forms (e.g., rotated K), or return to the E species. − The mechanism and rate constant of the ESIPT reactions depend on the PESs of the E* and K* tautomers in the first electronically first excited single state (S 1 ). , The presence or absence of barriers for both processes in S 0 and S 1 opens the possibility of controlling the related spectroscopy and dynamics. ,− Thus, for a PES without an energy barrier between the wells of E* and K* species, the ESIPT reaction is ultrafast (fs regime) and irreversible. , When the PES has a barrier in the conversion of E* to K*, the reaction may be reversible or irreversible but will be slower (ps–ns regime) than in the barrierless situation. ,− An accurate description of the reaction dynamics at the PESs of ESIPT processes in gas phase requires at least two reaction coordinates: (i) the proton motion within the corresponding IHB and (ii) the vibrational or torsional (angle) mode involving the distance between the partners; the angle between the involved moieties in the transfer could be important in the global reaction dynamics and subsequent processes. ,,, In the presence of an energy barrier in the PESs, the proton motion may occur via tunneling, which adds another (quantum) dimension to the reaction. In solution, the PESs might be complex, involving a solvent coordinate where its polarity and H-bonding could play an important role in shaping the spectroscopy and dynamics.…”