15min:
INTERNAL MIXING, PHENYL RING TORSION AND EXCITONIC INTERACTION IN DIPHENYLMETHANE.

NATHAN R. PILLSBURY, JAIME A. STEARNS, CHRISTIAN W. MÜLLER, ALOKE DAS, TALITHA M. SELBY AND TIMOTHY S. ZWIER, Department of Chemistry, Purdue University, West Lafayette, IN 47907-2084.

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The close proximity of two identical ultraviolet chromophores render diphenylmethane~(DPM) an interesting case for the study of the dependence of excitonic coupling on the distortion along low-frequency large-amplitude vibrational coordinates, in particular the phenyl ring torsional coordinates present in~DPM.

We have studied the fluorescence excitation spectrum and several single vibronic level fluorescence~(SVLF) spectra of the A1B(\mathrmS1) leftarrow X1A(\mathrmS0) and the B1A(\mathrmS2) leftarrow X1A(\mathrmS0) transition of~DPM cooled in a supersonic jet.

The band in the excitation spectrum blue-shifted by~123 \mathrmcm-1 from the \mathrmS1 leftarrow \mathrmS0 origin was assigned to the \mathrmS2 leftarrow \mathrmS0 origin. Its SVLF spectrum shows two-region fluorescence reminiscent of that previously observed in the gas-phase and supersonic jet spectra of naphthalene1 and~ovalene2. The high-energy region of this \mathrmS2~00~SVLF spectrum was tentatively assigned to transitions originating in vibrationally excited levels of the \mathrmS1~state. This finding indicates the presence of efficient internal mixing of the \mathrmS2~00 level with the sparse manifold of \mathrmS1 vibronic background levels. The quantum number changes in the non-totally symmetric torsional mode~(see figure) upon internal mixing suggest that additional to the internal conversion transitions accounted for by the Jortner-Berry Delta v = \pm 1 rule higher order vibronic mechanisms3 have to be considered as well.

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(1) S.~M.~Beck, D.~E.~Powers, J.~B.~Hopkins and R.~E.~Smalley, J.~Chem. Phys. , \textbf1980, 73 , 2019.
(2) A.~Amirav, U.~Even and J.~Jortner, J.~Chem. Phys. , \textbf1981, 74 , 3745.
(3) B.~Scharf, Chem. Phys. , \textbf1975, 7 , 478.