2006
DOI: 10.1021/jp054426h
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Cavity Ring-Down Spectroscopy of the Torsional Motions of 1,4-Bis(phenylethynyl)benzene

Abstract: The torsional motions of jet-cooled 1,4-bis(phenylethynyl)benzene (BPEB), a prototype molecular wire, were studied using cavity ring-down spectroscopy in the first UV absorption band (316-321 nm). The torsional spectrum of 1,4-bis(phenylethynyl)-2,3,5,6-tetradeuteriobenzene was also recorded in the gas phase. Both spectra were successfully simulated using simple cosine potentials to describe the torsional motions. The ground-state barrier to rotation was estimated to be 220-235 cm(-1), which is similar to that… Show more

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Cited by 73 publications
(81 citation statements)
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“…24,25 In general, transient absorption provides information on the time dependent response due to the population dynamics and/or conformational changes in the excited electronic states. However, any involvement of the Franck-Condon active vibrational modes remains invisible under the broad excited state absorption bands, which makes it difficult to elucidate the structural vibrations involved during the time dependent nuclear dynamics.…”
Section: Urls Measurementsmentioning
confidence: 99%
See 1 more Smart Citation
“…24,25 In general, transient absorption provides information on the time dependent response due to the population dynamics and/or conformational changes in the excited electronic states. However, any involvement of the Franck-Condon active vibrational modes remains invisible under the broad excited state absorption bands, which makes it difficult to elucidate the structural vibrations involved during the time dependent nuclear dynamics.…”
Section: Urls Measurementsmentioning
confidence: 99%
“…21,24 In the ground state, the rotational barrier around the sp 2 -sp CC single bond is very low; it was determined by Greaves et al to be 220-235 cm 1 from a jet spectroscopy experiment, and this number agrees with the AM1 calculations of Levitus (0.5 kcal/mol = 180 cm 1 ). 25,26 Therefore, all rotamers ranging from planar to twisted forms are likely to co-exist at room temperature, resulting in electronic transitions at different energies. However, in the excited state, the energy difference between the planar and the twisted conformation is believed to be much larger: 15 kcal/mol.…”
Section: Introductionmentioning
confidence: 99%
“…[5][6][7][8] Different research groups have investigated the use of PAEs and hyperbranched PAEs as molecular wires, OLEDs, OSCs, OTFTs and fluorescent chemical sensors. [9][10][11][12][13][14] The interesting electronic properties exhibited by PAEs can be related to the axial symmetry of ethynylene groups, which allows to maintain the conjugation (note that between adjacent aryl groups at different relative orientations rotational barriers are as small as 1 kcal mol -1 in these cases) [15][16][17][18][19][20] across the whole molecular backbone.…”
Section: Introductionmentioning
confidence: 99%
“…17 The increase in the delocalization of the LUMO orbital could be achieved by the introduction of ethynylene groups (-C≡C-) as a bridge between the three aromatic rings; in fact the ethynylene group, due to its axial symmetry, could allow to extend the conjugation to adjacent arylene groups. [27][28][29][30][31][32] Note also that the actual synthesis of s-tetrazine ethynylene derivatives is possible through cross-coupling reactions on some s-tetrazine compounds (compounds a and b in Chart 1), as shown by NovĂĄk and Kotschy, 33 though we are not aware of any attempt for (ArCC) 2 Tz compounds.…”
mentioning
confidence: 99%