2002
DOI: 10.1021/jp027198p
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Photoexcitation and Electron Transfer Properties of Rod- and Coil-Type Oligo(thienylene−ethynylene)s

Abstract: Photoexcitation and electron-transfer properties of two series of oligo(thienylene−ethynylene)s, in which thiophene rings were connected with ethynylene groups at 2,5 or 2,3 positions (nαTE or nβTE; n denotes the number of the repeating unit), have been studied. From MO calculations and steady-state absorption spectra, expanded π-electron systems were expected for rod-type nαTE in the ground states, while limited π-electron systems were expected for coil-type nβTE. On the other hand, because nβTE shows a subst… Show more

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Cited by 10 publications
(24 citation statements)
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“…These lifetimes probed at emission maxima are found to be single and two exponential in CHX and THF, respectively. The half-lives within a few hundred picoseconds were roughly in agreement with those in oligo­(thienyl ethynylene)­s (∼0.31 ns), suggesting that this part of emission is mainly contributed by the (TE) n chromophore. The long-lifetime emission only observed in THF is assumed to derive from a symmetry-broken excited state because of the fast solvation effect in polar THF, whereas there almost no solvation occurred in nonpolar CHX. , The following femtosecond time-resolved transient absorption measurements further help to identify the solvent-dependent excited state dynamical behaviors.…”
Section: Resultssupporting
confidence: 74%
“…These lifetimes probed at emission maxima are found to be single and two exponential in CHX and THF, respectively. The half-lives within a few hundred picoseconds were roughly in agreement with those in oligo­(thienyl ethynylene)­s (∼0.31 ns), suggesting that this part of emission is mainly contributed by the (TE) n chromophore. The long-lifetime emission only observed in THF is assumed to derive from a symmetry-broken excited state because of the fast solvation effect in polar THF, whereas there almost no solvation occurred in nonpolar CHX. , The following femtosecond time-resolved transient absorption measurements further help to identify the solvent-dependent excited state dynamical behaviors.…”
Section: Resultssupporting
confidence: 74%
“…Pd(0) is inserted into the C−Hal bond of R The relatively rigid conjugated OTE chains 3 (X=S) soon become (n≥4) insoluble unless solubilizing side chains are attached. Therefore, alkyl, 11,13,14,18,19,[21][22][23][25][26][27][28][31][32][33] aryl, 17 alkoxy 34 or alkylsulfanyl 34 groups are normally attached to one or both free positions of the thiophene rings.…”
Section: Methodsmentioning
confidence: 99%
“…In comparison with their corresponding OTEs, the obvious red-shift in absorption λ max of these molecular wires was achieved due to the introduction of truxene units to improve the effective conjugation length of the whole molecular wire. For example, the absorption λ max red-shifted about 77 nm for Tr(TE) 2 Tr , 49 nm for Tr(TE) 3 Tr , 39 nm for Tr(TE) 4 Tr , 22 nm for Tr(TE) 5 Tr relative to those of (TE) 2 (317 nm), of (TE) 3 (360 nm), of (TE) 4 (377 nm), and of (TE) 5 (400 nm), respectively. 4a, All PL spectra in solution showed a maximum peak with a shoulder on the red side. It was observed that the PL λ max in dilute THF solution red-shifted from Tr(TE) 2 Tr to Tr(TE) 6 Tr .…”
mentioning
confidence: 94%
“…Moreover, it was observed that both absorption and PL λ max of Tr(TE) 6 Tr red-shifted only 2 nm in comparison with those of Tr(TE) 5 Tr , which indicated that the saturation of the effective conjugation length of this series of molecular wires was achieved around Tr(TE) 6 Tr . Normally, the saturation of the effective conjugation length for OTEs is found at around the octomer range . The fluorescence quantum yields (Φ PL ) of these molecular wires in dilute THF solution were measured to be 0.25 for Tr(TE) 2 Tr , 0.22 for Tr(TE) 3 Tr , 0.20 for Tr(TE) 4 Tr , 0.20 for Tr(TE) 5 Tr , and 0.18 for Tr(TE) 6 Tr , respectively, using 9,10-diphenylanthracene as the standard .…”
mentioning
confidence: 99%