EVIDENCE FOR NONADIABATIC PROCESSES IN THE PHOTODISSOCIATION CAGE EFFECT OF VAN DER WAALS COMPLEXES OF $I_{2}$

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1992

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Ohio State University

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The mechanism of the one-atom cage effect in the photodissociation of I2-X complexes has been investigated, where X is Ar or Kr. Valentini and Cross1have demonstrated that excitation of I2Ar above the dissociation limit of the I2B state results in fluorescence from uncomplexed B state I2; the authors suggested that a purely mechanical mechanism is responsible. An alternative mechanism has been proposed by Beswick et.al.2 whereby the excitation places the complex not on the B state potential but on the repulsive Πu potential; coupling onto the B state and ejection of the Ar would then lead to the observed fluorescensce. The repulsive Πu state has been mapped by Tellinghuisen3, and it carries a transition intensity comparable to that for the B state in the spectral region near the B state dissociation limit. In order to distinguish between the possible mechanisms we have conducted high resolution laser induced absoption and fluorescence measurements on I2-Ar and I2-Kr in the bound region of the B state. In particular this allows us to observe that excitation of I2-Ar or I2-Kr to the Πu state, between the relatively sharp bound state B X transitions, induces a significant continuous fluorescence baseline. The fluorescence is red-shifted suggesting that it originates from B state I2. These results completely support the very specific mechanism proposed by Beswick et. al. Furthermore it is observed that a considerably higher efficiency is exhibited by Kr than Ar for the ``one-atom cage effect”, which is consistent with the virtually complete quenching of fluorescence observed upon excitation to the bound B state levels of I2-Kr. The observed one-atom cage effect is thus accomplished via the mixing of electronic states of I2 induced by the van der Waals complex partner. Given the T-shaped structure of these complexes this appears to be a mechanism for effectively coupling perpendicular nuclear motions. The efficiency of the processes will be discussed.

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  1. J.J. Valentini and J.B. Cross, J. Chem. Phys. 77, 572(1982). 2. J.A. Beswick, R. Monol, J.-M. Philippoz and H. van denBergh, J. Chem. Phys. 86, 3965 (1987). 3. J. Tellinghuisen, J. Chem. Phys. 58, 2821 (1973).

Author Institution: Department of Chemistry, Harvard University

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