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Photochemistry and Photophysics of Coordination Compounds

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<strong>Photochemistry</strong> <strong>and</strong> <strong>Photophysics</strong> <strong>of</strong> <strong>Coordination</strong> <strong>Compounds</strong>: Rhodium 247<br />

Table 1 Rate constants for charge recombination following electron transfer from DNAbound,<br />

photoexcited donors to ∆-Rh(phi)2(bpy) 3+ a<br />

Donor DNA krec [10 9 s –1 ] –∆G ◦ [V]<br />

∆-Ru(phen)2(dppz) 2+ Calf thymus 9.2 1.66<br />

rac-Ru(bpy)2(dppz) 2+ Calf thymus 7.1 1.69<br />

∆-Ru(dmp)2(dppz) 2+ Calf thymus 11 1.59<br />

∆-Ru(phen)2(F2dppz) 2+ Calf thymus 7.7 1.68<br />

rac-Ru(phen)2(Me2dppz) 2+ Calf thymus 9.2 1.67<br />

∆-Os(phen)2(dppz) 2+ Calf thymus 11 1.21<br />

Λ-Ru(phen)2(dppz) 2+ Calf thymus 4.5<br />

∆-Ru(phen)2(dppz) 2+ Poly-d(AT) 7.4<br />

∆-Ru(phen)2(dppz) 2+ Poly-d(GC) 0.21<br />

a Based on [144]<br />

presence <strong>of</strong> Ru(III) oxidized donor. The rate constants for charge recombination<br />

process (krec) were obtained from the decay <strong>of</strong> this signal. The data<br />

for seven donor–acceptor pairs are given in Table 1. Within this series, the<br />

driving force (∆G ◦ ) is comparable but the donors vary with respect to intercalating<br />

lig<strong>and</strong>, ancillary lig<strong>and</strong>s, chirality, <strong>and</strong> metal center. Despite such<br />

a range <strong>of</strong> chemical properties, the rate observed is centered around 10 10 s –1 .<br />

A significant difference in rate is observed, however, when the absolute<br />

configuration <strong>of</strong> the donor is varied. For the right-h<strong>and</strong>ed ∆-Ru(phen)2dppz 2+<br />

the value is 2.5 times higher with respect the left-h<strong>and</strong>ed enantiomer indicating<br />

a deeper stacking <strong>of</strong> this complex into the double helix. This result,<br />

according to the authors, clearly suggests that the electron transfer process<br />

required the intervening aromatic base pairs. The notion <strong>of</strong> highly efficient<br />

ET through the stack <strong>of</strong> DNA base is also strongly supported by the finding<br />

that the largest change in electron transfer rate is observed when the sequence<br />

<strong>of</strong> the DNA bridge is changed: for the same donor <strong>and</strong> acceptor reactants the<br />

rate with poly d(AT) is 30 times higher than with poly d(GC). This is an importantresultthatindicatesthattheπ-stacked<br />

bases <strong>of</strong> the DNA provide an<br />

effective pathway for electron transfer reactions. However, the crucial point <strong>of</strong><br />

this study that involves an untethered Ru/DNA/Rh system concerns the distances<br />

over which fast ET occurs. The question is: do the donor <strong>and</strong> acceptor<br />

complexes contact each other, or does electron transfer occur at long range?<br />

Two models were considered by the authors to interpret the experimental results:<br />

i) a cooperative binding model with ET over short D–A distance <strong>and</strong><br />

ii) a r<strong>and</strong>om binding model with ET over long distances. On the basis <strong>of</strong><br />

DNA photocleavage experiments, the first hypothesis was reject in favor <strong>of</strong><br />

a rapid long range ET with a shallow distance dependence [160]. On the other<br />

h<strong>and</strong>, soon thereafter, Barbara [161] reinterpreted the experimental results on<br />

a quantitative basis using computational simulation procedures <strong>and</strong> demon-

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