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The dissociative ionization dynamics of excited electronic states of the xenon dimer, Xe2, have been studied using velocity map ion imaging (VMI). A one-colour, (2+1) resonant excitation scheme was employed to first excite and then ionize selected vibrational levels of the Xe2 6p 2[1/2]0 0g+ Rydberg state. Cationic fragments were then detected by the VMI. The data provide an outstanding example of the reflection principle in photodissociation with the full nodal structure of the Rydberg state wavefunctions clearly observed in the final Xe+ kinetic energy distributions without the need for scanning the excitation energy. Fitting of the observed distributions provides detailed and precise information on the form of the Xe2+ I(1/2g) potential energy curve involved which is in excellent agreement with the results of photoelectron imaging studies [Shubert and Pratt, J. Chem. Phys. 134, 044315 (2011) ]. Furthermore, the anisotropy of the product angular distributions yields information on the evolution of the electronic character of the ionic state with internuclear separation, R. The combination of the nature of dissociative ionization and the extent of the bound state wavefunctions provide information over an unusually wide range of internuclear separation R (ΔR > 0.75 Å). This would normally require scanning over a considerable energy region but is obtained in these studies at a fixed excitation energy. [ABSTRACT FROM AUTHOR]

The photodissociation dynamics of Au-Xe leading to Xe+ formation via the Ξ1/2-X2Σ+ (v′, 0) band system (41 500-41 800 cm-1) have been investigated by velocity map imaging. Five product channels have been indentified, which can be assigned to photoinduced charge transfer followed by photodissociation in either the neutral or the [Au-Xe]+ species. For the neutral species, charge transfer occurs via a superexcited Rydberg state prior to dissociative ionization, while single-photon excitation of the gold atom in Au+-Xe accesses an (Au+)*-Xe excited state that couples to a dissociative continuum in Au-Xe+. Mechanisms by which charge transfer occurs are proposed, and branching ratios for Xe+ formation via the superexcited Rydberg state are reported. The bond dissociation energy for the first excited state of Au+-Xe is determined to be ∼9720 ± 110 cm-1. [ABSTRACT FROM AUTHOR]

Toluene-X van der Waals clusters (where X=Ne, Ne2, Ar, Ar2, Kr, Xe) have been investigated by fluorescence excitation spectroscopy in the region of the S1-S0 transition. With the exception of Xe, for each rare-gas studied, we have assigned cluster transitions in the region of all the strong monomer vibrational bands up to 1000 cm-1 above the origin band. We have further investigated the S1 relaxation dynamics for each vibrational level of each complex, via their fluorescence decay profiles. Clustering with neon has little appreciable effect on the vibrationless S1 lifetime. By contrast, the clusters with argon and krypton exhibit markedly shorter fluorescence lifetimes compared with the monomer. The effect is so severe in the case of toluene-Xe clusters that no fluorescence signals were observed. We interpret these results in terms of an external heavy atom effect in which the rate of intersystem crossing in toluene is influenced by the cluster partner. For clusters built upon excited S1 vibrational levels, the situation is potentially complicated by intramolecular vibrational redistribution and vibrational predissociation (VP). The majority of the fluorescence decay profiles were satisfactorily modeled using single exponential decays. The emission following pumping of the 371 level in the toluene-Kr cluster, however, is an exception. We have modeled the decay of this level with a simple kinetic scheme including VP and determined a predissociation rate of (1.04±0.54) × 107 s-1. [ABSTRACT FROM AUTHOR]

The photodissociation dynamics of Xe2 Rydberg states in the 76,900–80,000 cm−1 region have been studied using a combination of resonance enhanced multi-photon ionization and velocity map imaging. By monitoring photodissociation product channels as a function of excitation energy, several localized and long range perturbations of the excited states have been identified. In addition, several new band systems have been observed and assigned as the Xe2 5d 2[1/2]0°  ← X , 5d 2[1/2]1°  ← X , 5d 2[3/2]2°  ← X , and 5d 2[7/2]3°  ← X transitions. [ABSTRACT FROM AUTHOR]