1991
DOI: 10.1021/j100163a002
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Intramolecular charge shift following bimolecular reductive quenching of a rhodium(III) polypyridine-diquat dyad

Abstract: The Rh(NN)$+-w+ dyad, which contains a Rh(II1) polypyridine moiety (Rh(NN)f+) and a N,N'-bridged diquatemarized 4,4'dimethyl-2,2'-bipyridine (p) as covalently linked components, has been synthesized and used in the study of intramolecular electron transfer. The study, performed by laser flash photolysis, makes use of a relatively unconventional reaction scheme. First, bimolecular electron-transfer quenching of the Rh(NN)t+-localized excited state of the dyad (using 1,2,3-trimethoxybenzene as external reductant… Show more

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Cited by 6 publications
(3 citation statements)
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“…The distribution of molecules between the "remote" and "adjacent" excited states is given by a Boltzmann relationship and will depend upon the energy difference between them. If equilibrium is rapidly established on the electron transfer time scale, the observed rate constant for forward charge transfer (k°bs) is approximated as the average of the rate constant for charge transfer from the two states, weighted by their populations a and a -1, eq 13. k°bs = kf(a) + kT;m(a -1) (13) Considering the above arguments, our observation of a discrete "break" point in the forward charge transfer kinetics, between complexes 1,2,3-x-MV and 4, 5-x-MV, suggests that the relative populations of the "remote" and "adjacent" MLCT states change from predominantly "adjacent" in l-x-M through 3-x-MV to predominantly "remote" in 4-x-MV and 5-x-MV. One would expect the rate constant for charge transfer from the remote ligand, by either a through-bond or through-space mechanism, to be slow relative to that from the adjacent ligand, since both mechanisms necessarily involve a larger number of intervening bonds or greater separation distance.…”
Section: Discussionmentioning
confidence: 99%
“…The distribution of molecules between the "remote" and "adjacent" excited states is given by a Boltzmann relationship and will depend upon the energy difference between them. If equilibrium is rapidly established on the electron transfer time scale, the observed rate constant for forward charge transfer (k°bs) is approximated as the average of the rate constant for charge transfer from the two states, weighted by their populations a and a -1, eq 13. k°bs = kf(a) + kT;m(a -1) (13) Considering the above arguments, our observation of a discrete "break" point in the forward charge transfer kinetics, between complexes 1,2,3-x-MV and 4, 5-x-MV, suggests that the relative populations of the "remote" and "adjacent" MLCT states change from predominantly "adjacent" in l-x-M through 3-x-MV to predominantly "remote" in 4-x-MV and 5-x-MV. One would expect the rate constant for charge transfer from the remote ligand, by either a through-bond or through-space mechanism, to be slow relative to that from the adjacent ligand, since both mechanisms necessarily involve a larger number of intervening bonds or greater separation distance.…”
Section: Discussionmentioning
confidence: 99%
“…The simple chromophore-quencher system 24 also contains a quaternarized electron acceptor attached to a Rh(III) polypyridine unit. This dyad was designed [112] to study intramolecular charge shift processes, using a photochemical inter/intramolecular reaction scheme of the type shown in Eqs. 15-19.…”
Section: Triads and Other Complex Systemsmentioning
confidence: 99%
“…The rate constants of all the processes in the above scheme have been experimentally determined, except for that of Eq. 17, inferred from experiments on appropriate model rhodium systems (without DQ pendant unit) [112]. In particular, the intramolecular charge shift process (Eq.…”
Section: Triads and Other Complex Systemsmentioning
confidence: 99%