Photochemistry and Photophysics of Coordination Compounds
Photochemistry and Photophysics of Coordination Compounds
Photochemistry and Photophysics of Coordination Compounds
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126 S. Campagna et al.<br />
With increasing temperature, the emission lifetime (Fig. 8) <strong>and</strong> quantum<br />
yield decrease [1, 4, 6, 8, 32, 61–79]. This behavior may be accounted for by<br />
a stepwise term <strong>and</strong> two Arrhenius terms [1–3]:<br />
B<br />
1/τ =k0 +<br />
1+exp[C(1/T –1/TB)] + A1 exp(– ∆E1/RT)<br />
+ A2 exp(– ∆E2/RT). (1)<br />
The value <strong>of</strong> the various parameters is somewhat dependent on the nature<br />
<strong>of</strong> the solvent. In propionitrile–butyronitrile (4 : 5 v/v) the values are as<br />
follows [70, 71]: k0 = 2 × 10 5 s –1 ; B = 2.1 × 10 5 s –1 ; A1 = 5.6 × 10 5 s –1 ; ∆E1 =<br />
90 cm –1 ; A2 = 1.3 × 10 14 s –1 ; ∆E2 = 3960 cm –1 .Includedink0 are the radiative<br />
k0(r) <strong>and</strong> nonradiative k0(nr) rate constants at 84 K. The stepwise term B is<br />
due to the melting <strong>of</strong> the matrix (100–150 K) <strong>and</strong> corresponds to the coming<br />
into play <strong>of</strong> vibrations capable <strong>of</strong> facilitating radiationless deactivation [8, 71].<br />
Inthesametemperaturerangearedshift<strong>of</strong>∼ 1000 cm –1 is observed in the<br />
maximum <strong>of</strong> the emission b<strong>and</strong>, <strong>and</strong> it is mainly attributed to reorganization<br />
<strong>of</strong> solvent molecules around the excited state in fluid solution before<br />
emission takes place [8, 71]. The Arrhenius term with A1 = 5.6 × 10 5 s –1 <strong>and</strong><br />
∆E1 = 90 cm –1 is thought to correspond to the thermal equilibration with<br />
a level lying at slightly higher energy <strong>and</strong> having the same electronic nature<br />
(so it would be a fourth MLCT state [6], considering the lowest-lying MLCT<br />
state is made <strong>of</strong> three sublevels as described before). The second Arrhenius<br />
term corresponds to a thermally activated surface crossing to an upper-lying<br />
3 MC level which undergoes fast deactivation. Identification <strong>of</strong> this higher<br />
level as a 3 MC state is based upon the observed photosubstitution behavior<br />
at elevated temperatures [61], consistent with established photoreactivity<br />
patterns for d 6 metal complexes [17, 52].<br />
Experiments carried out with [Ru(bpy)3] 2+ <strong>and</strong> [Ru(bpy-d8)3] 2+ in H2O<br />
<strong>and</strong> D2O [61, 80, 81] indicate that k0(nr) is sensitive to deuteration, as expected<br />
for a weak-coupled radiationless process [6, 82–84]. By contrast, A2<br />
is insensitive to deuteration, supporting a strong-coupled (surface crossing)<br />
deactivation pathway, which may be related to the observed photosensitivity.<br />
It should be noted that the decrease in lifetime on melting has also been explained<br />
on the basis <strong>of</strong> the energy gap law because <strong>of</strong> the corresponding red<br />
shift in the emission b<strong>and</strong> [6].<br />
Finally, it should be noted that at 77 K the emission spectrum <strong>of</strong><br />
[Ru(bpy)3] 2+ , as well as that <strong>of</strong> most Ru(II) polypyridine complexes, exhibits<br />
a vibrational structure (see Fig. 7). This structure is assigned to the vibrational<br />
progression, <strong>and</strong> its energy spacing is about 1300 cm –1 ,equivalentto<br />
the C – N<strong>and</strong>C– C stretching energy <strong>of</strong> the aromatic rings, thus indicating<br />
that such stretchings are the dominant accepting modes for deactivation <strong>of</strong><br />
the 3 MLCT state.