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0011473170
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note
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1 The difference does not represent substantial deactivation of PDI* to the ground-state competing with PDI*-pep-Fb → PDI-pep-Fb* energy transfer; the high efficiency of the latter process is also born out by the static fluorescence measurements.
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1 This result reflects the relatively weak electronic interactions in the dyads. (a) Hsiao, J.S.; Krueger, B.P.; Wagner, R.W.; Johnson, T.E.; Delaney, J.K.; Mauzerall, D.C.; Fleming, G.R.; Lindsey, J.S.; Bocian, D.F.; Donohoe, R.J. J. Am. Chem. Soc. 1996, 118, 11181-11193. (b) Li, F.; Gentemann, S.; Kalsbeck, W.A.; Seth, J.; Lindsey, J.S.; Holten, D.; Bocian, D.F. J. Mater. Chem. 1997, 7, 1245-1262.
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1 This result reflects the relatively weak electronic interactions in the dyads. (a) Hsiao, J.S.; Krueger, B.P.; Wagner, R.W.; Johnson, T.E.; Delaney, J.K.; Mauzerall, D.C.; Fleming, G.R.; Lindsey, J.S.; Bocian, D.F.; Donohoe, R.J. J. Am. Chem. Soc. 1996, 118, 11181-11193. (b) Li, F.; Gentemann, S.; Kalsbeck, W.A.; Seth, J.; Lindsey, J.S.; Holten, D.; Bocian, D.F. J. Mater. Chem. 1997, 7, 1245-1262.
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0011382821
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note
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s the static dielectric constant (2.38 for toluene and 37.4 for acetonitrile).
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21
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0011440302
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note
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s ∼ 0.05 eV for toluene and ∼0.7 eV for acetonitrile. Thus, the total reorganization energy is estimated to be λ ∼ 0.4 eV for the charge-transfer and charge-recombination reactions in toluene and λ ∼ 1.1 eV in acetonitrile.
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30
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0011475870
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note
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+ → PDI-pep-Fb* charge recombination in toluene (half-filled circle and square in Figure 8A); the trend is followed by that pair in acetonitrile (Figure 8B).
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