Abstract

The reaction between He^{+} and CH_{3}F forming predominantly CH_{2}^{+} and CHF^{+} has been studied at collision energies E_{coll} between 0 and k_{B}·10 K in a merged-beam apparatus. To avoid heating of the ions by stray electric fields, the reaction was observed within the orbit of a highly excited Rydberg electron. Supersonic beams of CH_{3}F and He(n) Rydberg atoms with principal quantum number n=30 and 35 were merged and their relative velocity tuned using a Rydberg-Stark decelerator and deflector, allowing an energy resolution of 150mK. A strong enhancement of the reaction rate was observed below E_{coll}/k_{B}=1 K. The experimental results are interpreted with an adiabatic capture model that accounts for the state-dependent orientation of the polar CH_{3}F molecules by the Stark effect as they approach the He^{+} ion. The enhancement of the reaction rate at low collision energies is primarily attributed to para-CH_{3}F molecules in the J=1, KM=1 high-field-seeking states, which represent about 8% of the population at the 6K rotational temperature of the supersonic beam.

Highlights

  • The reaction between Heþ and CH3F forming predominantly CHþ2 and CHFþ has been studied at collision energies Ecoll between 0 and kB · 10 K in a merged-beam apparatus

  • In this Letter we present, with the example of the reaction between Heþ and CH3F, experimental results at very low collision energies on barrier-free exothermic reactions between ions and polar molecules, which are the class of reactions for which the strongest low-temperature effects are expected [24,25,26,27,28]

  • We report the observation of a large enhancement of the reaction rate at collision energies Ecoll

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Summary

Introduction

The reaction between Heþ and CH3F forming predominantly CHþ2 and CHFþ has been studied at collision energies Ecoll between 0 and kB · 10 K in a merged-beam apparatus. The method combines the advantages of merged-beam approaches to study neutral-neutral reactions at low collision energies [6,9,11] with those offered by Rydberg atoms and molecules, e.g., the ease of manipulation of their translational motion with inhomogeneous electric fields [41,42,43].

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