Based
on the results of fs-TAS of 1-H+ (see above),
the emission of 1-H+ at 380 nm is ascribable
to the singlet π–π* excited state of its tpphz
ligand, which is also responsible for the photocatalysis of substrate
oxidation by 1-H+. Normally, a higher excited
state such as the S2 state [1(π–π*)*]
undergoes relaxation to form a lower excited state such as the S1 state (1MLCT*) through thermal IC and finally
reaches the lowest triplet excited state of T1 (3MLCT*) through intersystem crossing, which is radiatively relaxed
to the ground state ( Figure 11a), according to Kasha’s rule. (17) Not the lowest singlet excited state (S1), i.e., 1MLCT*, but a higher singlet excited state
(S2), i.e., 1(π–π*)*, of 1-H+ performs the photocatalytic oxidation of organic
substrates, that is, an example of anti-Kasha photocatalysis. (17) A particularly unique feature of this system
is that protonation at the vacant diimine site of the tpphz ligand
in 1-H+ induces emission from the S21(π–π*)* state and oxidation of external
organic substrates (Figure 11b). Probably, due to the protonation at the vacant diimine
site of the tpphz ligand, spin density in the 1(π–π*)*
excited state is biased toward the protonated diimine site, which
retards the IC to 1MLCT*, since the spin density in the 1MLCT* mainly localizes at the RuII center and the
other diimine site of the tpphz ligand bonded to the RuII center. (53) Insufficient orbital overlapping
in the excited electronic structures is well-known to be important
for anti-Kasha chromophores. (20a)
