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Generation and characterization of highly vibrationally excited molecular beam.

A simple method to generate and characterize a pure highly vibrationally excited azulene molecular beam is demonstrated. Azulene molecules initially excited to the S4 state by 266-nm UV photons reach high vibrationally excited levels of the ground electronic state upon rapid internal conversion from the S4 electronically excited state. VUV laser beams at 157 and 118 nm, respectively, are used to characterize the relative concentrations of the highly vibrationally excited azulene and the rotationally and vibrationally cooled azulene in the molecular beam. With a laser intensity of 34 mJ/cm2, 75% of azulene molecules absorb a single 266-nm photon and become highly vibrationally excited molecules. The remaining ground-state azulene molecules absorb two or more UV photons, ending up either as molecular cations, which are repelled out of the beam by an electric field, or as dissociation fragments, which veer off the molecular-beam axis. No azulene without absorption of UV photons is left in the molecular beam. The molecular beam that contains only highly vibrationally excited molecules and carrier gas is useful in various experiments related to the studies of highly vibrationally excited molecules.

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Controlling factors in electron and energy transfer reactions on silica gel surfaces.

Energy and electron transfer reactions between co-adsorbed molecules on silica gel have been studied using nanosecond time-resolved diffuse reflectance laser flash photolysis. The systems under investigation are anthracene and 9-carboxylic acid anthracene co-adsorbed with azulene, which undergo both triplet-triplet energy transfer and electron transfer from azulene to the anthracene radical cation following laser excitation. The decay traces have been analysed using a model which assumes a log gaussian distribution of rate constants and the methodology behind the optimisation of the fitting parameters is described. Bimolecular rate constants for energy and electron transfer between anthracene (and its derivative) and azulene have been obtained. Ground state association between anthracene and azulene has been observed, and an equilibrium constant for the process determined. The kinetic data is corrected for these ground state association effects which reduce the free azulene concentration. For both systems and for both the energy and electron transfer processes, analysis of the quenching data yields the same quenching constant. This indicates that the rate of reaction of anthracene (and the 9-carboxylic acid anthracene) on silica gel is predominantly governed by the rate of diffusion of the quencher.

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Synthesis, stability and bonding situation of tris-, bis- and mono[9-(azuleno[1,2-b]thienyl)]methyl cations.

Stable tris-, bis- and mono[9-(azuleno[1,2-b]thienyl)]methyl cations (7a, 8a and 9a) and their derivatives, with a 6-isopropyl substituent on each azuleno[1,2-b]thiophene ring (7b, 8b and 9b) were prepared by the hydride abstraction reaction of the corresponding methane derivatives. The bonding situation of these compounds including the methane derivatives was examined by analysis of the 3J(H,H) values for the seven-membered ring from the 1H NMR spectra. The methane derivatives exhibited a significant alternating pattern in the 3J(H,H) values, which indicated that the pi-system of the azulene core is perturbed by the fused thiophene ring, showing a tendency towards a localized heptafulvene substructure. The 3J(H,H) values of 7b and 8b in the seven-membered ring revealed that the alternating C-C bond lengths in the azulene core still existed. The cations 9a and 9b, which exhibited nearly equal 3J(H,H) values in the seven-membered ring, exhibit the development of a delocalized tropylium substructure in the azulene core. X-ray crystal analysis of 6-isopropylazuleno[1,2-b]thiophene revealed substantial bond-length alternation in the seven-membered ring. Significant bond-length equalization in the seven-membered ring was also confirmed by the X-ray crystal analysis of 9b. The stability of these carbocations was examined by measurement of the pKR+ values and the redox potentials, which revealed that the bond-length alternation in the azulene core does not significantly affect the stability of the carbocations.

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