Interestingly, this effect was inversely proportional to the energy
of the^3 MLCT state (E 00 in Tables III and IV). Therefore, the
energy gap between the ground state and the transition state of
the photochemical ligand substitution reaction (E 00 þDG6¼) is
not affected by the modification of the bipyridine ligand as much
1500
260
0.0
0.1
Quantum yield
0.2
0.3
0.4
0.5
280 300
te
Fe
Fr
320 340
0
500 Lifetime (ns)
1000
T (K)
FIG. 11. Temperature dependence of the emission yield (Fe), the life-
time (te), and the quantum yield of the photochemical ligand substitu-
tion reaction (Fr) of 3a in a degassed CH 3 CN solution. Copyright
2002 American Chemical Society.
3.2 3.4 3.6 3.8
T–1 (10^3 K–1)
2.8 3.0
8
10
In {(
fe
/te
) (s
–1
)}, In{(
fr
/t
) (se
–1
)}
12
In kr
In ke
14
16
FIG. 12. Arrhenius plots of the radiative decay rate (ke) and the reac-
tion rate of the photochemical ligand substitution reaction (kr) of3ain
a degassed CH 3 CN solution. Copyright 2002 American Chemical
Society.
156 HIROYUKI TAKEDAet al.