“…With the exception of a few compounds with high oxidation potentials and low excited-state energies, the experimental overall S 1 quenching rate constants
are found to be nearly collision-controlled in the gas phase ,,, or diffusion-controlled in the liquid phase. ,,,− However, all quenching pathways compete with relatively efficient intramolecular deactivation processes, and
values distinctly smaller than unity are commonly found under air-saturated conditions in solution. The first experimental studies were concerned with the multiplicity of the sensitizer product state, and it was shown that isc (eqs 50−53) is dominant over ic (eqs 54−56); i.e., oxygen quenching of S 1 states leads mainly to formation of a triplet state. ,− Brauer and Wagener , first provided clear evidence for overall singlet oxygen yields larger than unity, thus showing that the energy-transfer process 52 can significantly contribute to the deactivation of S 1 . These observations are obviously limited to molecules having a S 1 −T 1 energy gap larger than 94 kJ mol -1 , such as rubrene, ,,− heterocoerdianthrone, , tetracene, ,,, perylene, ,,, pyrene, ,,− chrysene, ,− 1,3-diphenylisobenzofuran, 1,6-diphenylhexatriene, fluoranthene, , a larg...…”