Three-State Feshbach Resonances Mediated By Second-Order Couplings

TL;DR

This paper provides an analytical framework for understanding three-state Feshbach resonances caused by second-order couplings, relevant in ultracold atomic and molecular collision processes, with general expressions for resonance characteristics.

Contribution

It introduces a general analytical model for three-state Feshbach resonances mediated by second-order couplings, including multiple intermediate states, extending previous simpler models.

Findings

Derived expressions for energy-dependent T-matrix modifications.

Analyzed how resonance positions and widths depend on coupling amplitudes.

Generalized the model to include multiple sequential off-resonant bound states.

Abstract

We present an analytical study of three-state Feshbach resonances induced by second-order couplings. Such resonances arise when the scattering amplitude is modified by the interaction with a bound state that is not directly coupled to the scattering state containing incoming flux. Coupling occurs indirectly through an intermediate state. We consider two problems: (i) the intermediate state is a scattering state in a distinct open channel; (ii) the intermediate state is an off-resonant bound state in a distinct closed channel. The first problem is a model of electric-field-induced resonances in ultracold collisions of alkali metal atoms [Phys. Rev. A 75, 032709 (2007)] and the second problem is relevant for ultracold collisions of complex polyatomic molecules, chemical reaction dynamics, photoassociation of ultracold atoms, and electron - molecule scattering. Our analysis yields general expressions for the energy dependence of the T-matrix elements modified by three-state resonances and the dependence of the resonance positions and widths on coupling amplitudes for the weak-coupling limit. We show that the second problem can be generalized to describe resonances induced by indirect coupling through an arbitrary number of sequentially coupled off-resonant bound states and analyze the dependence of the resonance width on the number of the intermediate states.