We present time-resolved measurements for the dissociative decay of NO2 in its ground electronic state using
pump laser pulses with durations of ca. 650 fs. The temporal evolution of the coherent wave packet is probed
by excitation to a Rydberg state and detection of the subsequent fluorescence. The main experimental result
is the observation of nonexponential decay, which is most pronounced at very low excess energies close to
the dissociation threshold. This is compared with the results of quantum dynamics calculations performed on
a recently calculated global potential energy surface. The measured decay curves are satisfactorily reproduced
by summation of many exponential decay terms e-knt, with the state-specific dissociation rates kn being
determined from the widths of resonance poles in the complex energy plane. The key theoretical result is the
observation that the calculated rates fluctuate by 1−2 orders of magnitude. These strong fluctuations are
responsible for the distinct nonexponential behavior. The smallest calculated rates just at threshold are of the
same order of magnitude, ca. 2 × 1010 s-1, as the experimental rates previously extracted from energy-resolved spectra.