2012
DOI: 10.1103/physrevb.86.199903
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Erratum: Ultrafast optical studies of ordered poly(3-thienylene-vinylene) films [Phys. Rev. B85, 235201 (2012)]

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Cited by 10 publications
(33 citation statements)
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“…In this picture PA 2 band may be a transition from the 1B u to another, higher two-photon state, so called kA g [26][27][28]. Although the exciton in t-(CH) x has characteristic PA bands similar to many other polymers in the π-conjugated polymer family, it is still unique because the photogenerated 1B u exciton decays within ~100 fs to a "dark", lower lying exciton (so called 2A g state) that is nonradiative [29][30][31][32][33][34]. The transient PM spectra and decay dynamics clearly show that the generation of 2A g exciton is at the expense of 1B u exciton.…”
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confidence: 99%
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“…In this picture PA 2 band may be a transition from the 1B u to another, higher two-photon state, so called kA g [26][27][28]. Although the exciton in t-(CH) x has characteristic PA bands similar to many other polymers in the π-conjugated polymer family, it is still unique because the photogenerated 1B u exciton decays within ~100 fs to a "dark", lower lying exciton (so called 2A g state) that is nonradiative [29][30][31][32][33][34]. The transient PM spectra and decay dynamics clearly show that the generation of 2A g exciton is at the expense of 1B u exciton.…”
mentioning
confidence: 99%
“…The transient PM spectra and decay dynamics clearly show that the generation of 2A g exciton is at the expense of 1B u exciton. Importantly, the 2A g , which is the lowest two-photon state, occurs below the 1B u in most non-luminescent polymers [29][30][31][32][33][34][35];…”
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confidence: 99%
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“…The absorption spectrum is broad with an absorption maximum at 560 nm, similar to previously reported results 9. It has been reported that P3HTV films are almost non‐fluorescent with a fluorescence quantum efficiency less than 0.02 %, presumably owing to the of 2 1 A g symmetry of the lowest‐lying excited state,10 from which the electronic transition to the 1 1 A g ground state is forbidden. However, we found that the fluorescence intensity of a film of concentrated rra‐P3HTV embedded in a poly(methyl methacrylate) (PMMA) matrix (rra‐P3HTV/PMMA film hereafter) is much brighter than that of the pure rra‐P3HTV film under 488 nm Ar ion laser excitation in a wide‐field fluorescence microscope (Figure S2 in the Supporting Information).…”
Section: Resultsmentioning
confidence: 99%
“…We have measured ultrafast dynamics of the primaryphotoexcitations in four typical polymers that represent both degenerate and non-degenerate ground state polymers. This includetrans-polyacetylene (DGS, low intrinsic PL efficiency) [44], polyfluorene (NDGS, high PL efficiency) [16], DPA (DGS, high PL efficiency) [45], and regio-random poly (thienylene-vinylene) (NDGS, low intrinsic PL efficiency) [46]. In all of these polymers, theexciton is the primary photoexcitation when the laser excitation photon energy is close to the absorption onset of polymers; in all casesexcitonic transition such as PA 1 is observed in the transient PM spectroscopy, havingdifferent dynamics.…”
Section: Methodsmentioning
confidence: 99%