2011
DOI: 10.1039/c1cp20539k
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Superexchange mediated energy transfer in zinc(ii) porphyrin–free base porphyrin dimers: comparison of m- and p-bis(phenylethynyl) phenylene linked dimers

Abstract: The singlet-singlet energy transfer rate in a new zinc(II) porphyrin-free base porphyrin dimer, having a m-bis(phenylethynyl)phenylene bridge, was found to be slower than that in the corresponding p-bis(phenylethynyl)phenylene-bridged dimer, despite the shorter donor-acceptor distance and pathway. The slower rate is interpreted as evidence for a major contribution of the superexchange mechanism.

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Cited by 14 publications
(10 citation statements)
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“…As described, excitation spectra could not detect any trance of intramolecular energy transfer, which can be usually confirmed by the fluorescence excitation spectra. 28 One of the possibilities is energy transfer between two PFV units which have different repeat numbers and that are connected via a 3PV unit in a polymer chain. Although polymers studied in this work have rather narrow distribution of molecular sizes, there should be some species, which consist of two different PFV units in their repeat numbers (for example, C 6 F 5 -(PFV) 8 -3PV-(PFV) 12 -C 6 F 5 ).…”
Section: Macromoleculesmentioning
confidence: 99%
“…As described, excitation spectra could not detect any trance of intramolecular energy transfer, which can be usually confirmed by the fluorescence excitation spectra. 28 One of the possibilities is energy transfer between two PFV units which have different repeat numbers and that are connected via a 3PV unit in a polymer chain. Although polymers studied in this work have rather narrow distribution of molecular sizes, there should be some species, which consist of two different PFV units in their repeat numbers (for example, C 6 F 5 -(PFV) 8 -3PV-(PFV) 12 -C 6 F 5 ).…”
Section: Macromoleculesmentioning
confidence: 99%
“…The short lifetime component can be associated to the characteristic time constant of the energy transfer, and the long lifetime component may be the decay of the excited free Ru. This suggests that the energy transfer rate from the excited Ru to TAPP is ∼1.8 × 10 9 s −1 , which is similar to through-space singlet energy transfer for donor-acceptor distances approaching 3.5-3.6Å [53,54]. In addition, the fs fluorescence up-conversion data (see Figure 6B) show a very fast decay of the Ru excited state with a characteristic time constant of 160 fs, providing a clear indication for static quenching.…”
Section: Ru-tapp Associationmentioning
confidence: 71%
“…One distinct character for TADPP2‐TT and TADPP3 is that their HOMOs and LUMOs show similar distributions not only on the DPP units, but also extending to the acetylene and part of the benzene core. Conjugation is then broken in the meta ‐substituted benzene core in which two atoms in the benzene core have no electron population in the calculated HOMOs and LUMOs . Furthermore, the frontier orbitals of TADPP2‐TT show that the 2,2′:5′2′′‐terthiophene moiety does not contribute to the first excited state, which suggests that TADPP2‐TT can be treated as a simple DPP dimer.…”
Section: Resultsmentioning
confidence: 99%
“…Conjugation is then broken in the meta-substituted benzene core in which two atoms in the benzene core have no electron population in the calculated HOMOsa nd LUMOs. [18] Furthermore, the frontier orbitals of TADPP2-TT show that the 2,2':5'2''-ter- In addition, the geometries of the excited states of TADPP2-TT and TADPP3 were optimized to determine the electronic coupling between branches. The corresponding bond lengths of the ground and excited states are showni nS ection S3 in the Supporting Information.…”
Section: Quantum Chemical Calculationsmentioning
confidence: 99%