Abstract
Building on our previous work on NO + Ar, this paper presents a complete set of orientation measurements and quantum mechanical calculations for the NO + Kr collision system, including both spin-orbit conserving and changing collisions, and both side-on (x-axis) and end-on (z-axis) orientations. While many of the trends observed in the oriented differential and integral scattering distributions, as well as in the spin-orbit branching fractions, are similar to the ones seen previously for NO + Ar, a direct comparison with the Ar data reveals subtle differences in the scattering dynamics, which we rationalise with the more extended attractive regions on the NO + Kr potential energy surfaces. High-impact parameter collisions that lead to low scattering angles in the spin-orbit conserving manifold are particularly sensitive to the topology in the attractive parts of the potential, whereas more impulsive, low-impact parameter trajectories, which sample the repulsive parts of the potential, produce very similar features in the oriented differential cross sections for the Ar and Kr systems, especially for spin-orbit changing collisions.
Highlights
The QM NO + He integral spin-orbit branching fractions for the j′ = 5.5e − 10.5e final rotational states are presented in Figure S1, along with the branching fractions for NO + Ar and NO + Kr
The calculations for the NO + He system were run at the same field strength as was used in the current experiments (9.2 kV/cm), using the potential energy surfaces of Yang and Alexander [1]
As discussed in the main text, this is due to the dominance of the repulsive core of the NO + He
Summary
1. Integral spin-orbit branching fractions for NO + He The QM NO + He integral spin-orbit branching fractions for the j′ = 5.5e − 10.5e final rotational states are presented, along with the branching fractions for NO + Ar and NO + Kr (these are the same QM fractions as shown in Figure 7 of the main text, plotted on a larger scale).
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