The fragmentation of van der Waals (vdW) complexes offers an opportunity for studying the half-collision dynamics in well-defined systems. In previous work from this laboratory, we have studied, 1 in real time, the dynamics of the "hair' and the "full" collision, but we had no results on the diatom-rare gas small vdW complexes. Iodine with rare gases I 2 -M (M =He, Ne, and Ar) are of particular interest for a number of reasons.First, the IrM vibrational dynamics are rather simple; an iodine stretch, and two van der Waals' stretch and bend modes. Second, from the pioneering work 2 on the spectroscopy, there is a wealth of data that provide the vibrational structure, geometry, and the photochemistry of these systems. Third, the I 2 real-time dynamics on the fs-ps time scale have already been reported. 3 Finally, unlike the case of large molecules, theory is quite advanced 4 for these smaller systems, and there is hope for a detailed understanding of IVR and vibrational predissociation. Real-time studies of large vdW complexes have been reported for isoquinoline, I tetrazine (in sl and So)' 5 phenoV cresoV perylene, 6 stilbene, 1 • 7 aniline, 8 and (N0) 2 (in S 0 ), 9 and only recently have results become available for the family of halogens. With nanosecond lasers, the lifetime of I CI-Ne in its A state was measured to be 3 ± 2 ns for v' = 14 by the Lester group. 10 As discussed below, other methods, such as linewidth measurements, have been used to deduce vibrational predissociation lifetimes.In this communication, we report direct picosecond measurements of the state-to-state rates obtained from real-time observation of fragment I! molecules in the reaction I *
1----AxOn the picosecond time scale, we observe the exponential buildup of nascent I! population, and the experiments show a slow "inverse" dependence on v', i.e., a slight decrease in the rate with increased v'. The results give the homogeneous width of the initial state, and establish the time scale for the dynamics in the channels, I! + Ar (vibrational predissociation, kv) and I + I + Ar (electronic predissociation, ke). The rise times measured in our experiments correspond to T = (kv + ke)-1 , and for the above reaction, n = 21 and 18 in the B state of I 2 (or Iz-Ar ). The binding energy oflz-Ar is known to be between 220 to 226 em-1 ; at the vibrational levels that we access in this experiment, this requires the redistribution of at least three quanta of energy from the iodine to the van der Waals bond in order to induce dissociation. (The geometry is not known from our experiments, but we draw it to be nonlinear, as suggested by previous work. 11 ) The experiments required a special care, because of inherent difficulties in preparing "clean" complexes ( usually much weaker than the parent species) with no background and at the same time detecting them with highenough sensitivity for state-to-state measurements on the picosecond time scale. The pump-probe scheme applied in these molecular beam experiments is similar to that used in earlier developm...