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See the Supporting Information for detail
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See the Supporting Information for detail.
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36
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68949087125
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In benzonitrile, the emission maximum of G1 was shifted to 660 nm, suggesting the highly polar nature of the emissive state.
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In benzonitrile, the emission maximum of G1 was shifted to 660 nm, suggesting the highly polar nature of the emissive state.
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37
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68949087126
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In CH2Cl2, pulsed laser irradiation (355 nm) of G1 gave a development of transient absorption maxima at 473, 525, and 560 nm, and their lifetime was ca. 27 μs. Almost the same transient absorption profiles were observed in benzonitrile, indicating little solvent effect on the excited states. In addition, an air-saturated CH2Cl2 or benzonitrile solution of G1 did not exhibit clear transient absorptions. These results suggest that the intermediate observed in these measurements is not an ICT state but a triplet state. A pathway from the Franck-Condon state of G1 to the triplet state is not elucidated yet, but the ICT state is assumed to be formed as a primary intermediate that gives the fluorescence and is transformed into the triplet state to some extent
-
2 or benzonitrile solution of G1 did not exhibit clear transient absorptions. These results suggest that the intermediate observed in these measurements is not an ICT state but a triplet state. A pathway from the Franck-Condon state of G1 to the triplet state is not elucidated yet, but the ICT state is assumed to be formed as a primary intermediate that gives the fluorescence and is transformed into the triplet state to some extent.
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39
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68949116889
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2/ εα) was neglected here because both the electron donor and acceptor are neutral molecules, and hence, the Coulomb interaction between them should be quite small.
-
2/ εα) was neglected here because both the electron donor and acceptor are neutral molecules, and hence, the Coulomb interaction between them should be quite small.
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