Long-range model of vibrational autoionization in core-nonpenetrating Rydberg states of NO

TL;DR

This paper presents a long-range theoretical model explaining vibrational autoionization in high-angular-momentum Rydberg states of nitric oxide, clarifying angular momentum exchange mechanisms and accurately predicting decay rates and ion state distributions.

Contribution

The study introduces a simplified long-range model for core-nonpenetrating Rydberg states that explains autoionization dynamics and decay rates, advancing understanding of vibrational autoionization mechanisms.

Findings

Explains angular momentum exchange in vibrational autoionization.

Accurately predicts decay rates for high-$ll$ Rydberg states.

Provides ion rotational state distribution predictions.

Abstract

In high orbital angular momentum ($\ell \geq 3$) Rydberg states, the centrifugal barrier hinders close approach of the Rydberg electron to the ion-core. As a result, these core-nonpenetrating Rydberg states can be well described by a simplified model in which the Rydberg electron is only weakly perturbed by the long-range electric properties (i.e., multipole moments and polarizabilities) of the ion-core. We have used a long-range model to describe the vibrational autoionization dynamics of high-$\ell$ Rydberg states of nitric oxide (NO). In particular, our model explains the extensive angular momentum exchange between the ion-core and Rydberg electron that had been previously observed in vibrational autoionization of $f$ ($\ell=3$) Rydberg states. These results shed light on a long-standing mechanistic question around these previous observations, and support a direct, vibrational mechanism of autoionization over an indirect, predissociation-mediated mechanism. In addition, our model correctly predicts newly measured total decay rates of $g$ ($\ell=4$) Rydberg states because, for $\ell\geq4$, the non-radiative decay is dominated by autoionization rather than predissociation. We examine the predicted NO$^+$ ion rotational state distributions generated by vibrational autoionization of $g$ states and discuss applications of our model to achieve quantum state selection in the production of molecular ions.