4.6 Article

CH3 Internal Rotation in the S0 and S1 States of 9-Methylanthracene

Journal

JOURNAL OF PHYSICAL CHEMISTRY A
Volume 113, Issue 11, Pages 2366-2371

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/jp808550r

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Funding

  1. Ministry of Education, Culture, Sports, Science, and Technology of Japan

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Fluorescence excitation spectra and dispersed fluorescence spectra of jet-cooled 9-methylanthracene-h(12) and -d(12) (9MA-h(12) and 9MA-d(12)) have been observed, and the energy levels of methyl internal rotation (CH3 torsion) in the S-0 and S-1 states have been analyzed. The molecular symmetry of 9MA is the same as that of toluene (G(12)). Because of two-fold symmetry in the pi system, the potential curve has six-fold barriers to CH3 rotation. In toluene, the barrier height to CH3 rotation V-6 is very small, nearly free rotation. As for 9MA-h(12), we could fit the level energies by potential curves with the barrier heights of V-6(S-0) = 118 cm(-1) and V-6(S-1) = 33 cm(-1). These barrier heights are remarkably larger than those of toluene and are attributed to hyperconjugation between the pi orbitals and methyl group. The dispersed fluorescence spectrum showed broad emission for the excitation of 08 + 386 cm(-1) band, indicating that intramolecular vibrational redistribution efficiently occurs, even in the vibronic level of low excess energy of the isolated 9MA molecule.

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