energies of these states can be controlled by systematic chemical
modification of the bipyridine and axial ligands. In doing so, the
energy gap between^3 MLCT and^3 LF states can be tuned. Such
modification effects are summarized as follows:
- Modification of the bipyridine ligand with introduction of elec-
tron-withdrawing (donating) groups at the 4,4^0 -positions
0
0
0
–1
–2
–3
1
1871 cm–1 2050 cm–1
2012 cm–1
2000 2100
Wavenumber (cm–1)
1900
–2
–8
–4
0
0
0.0
1.0
2.0
2 4 6 8 10
4 (a)
(b)
0
2
ΔAbsorbance
×^10
–2
ΔAbsorbance
×^10
–2
ΔAbsorbance
×^10
–2
ΔAbsorbance
×^10
–2
246810
Time (ms)
Time (ms)
0246810
Time (ms)
FIG. 10. TR-IR spectra of3ain a degassed CH 3 CN solution taken at
50 ns (a) and 5ms (b) after 355-nm laser excitation. The three small
figures are the decay traces for typical IR bonds. (Copyright 2002
American Chemical Society.)
RHENIUM(I) DIIMINE COMPLEXES 153