Abstract
Recent experimental works report observations of a significant vibrational dependence of the photoelectron angular distributions (PADs) recorded for the O2(X3Σg) ← O−2 (X2Πg) band. It is the aim of the theoretical model presented here to reproduce the experimental results, allow for a deeper insight into the mechanism of this process and explain the sensitivity of the PAD to vibronic coupling in the anion ground electronic state.
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