SU(3) orbital Kondo effect with ultracold atoms

TL;DR

This paper proposes a novel ultracold atom setup to realize the SU(3) orbital Kondo effect, demonstrating how impurity-fermion interactions lead to many-body phenomena analogous to condensed matter Kondo physics.

Contribution

It introduces a new scheme to observe the SU(3) orbital Kondo effect with ultracold atoms, including the formation of a Kondo singlet and anisotropic interactions.

Findings

Universal Kondo temperature dependence on scattering volume and Fermi wave vector

Formation of a Kondo singlet at zero temperature

Potential observation via atom loss or radio-frequency spectroscopy

Abstract

We propose a simple but novel scheme to realize the Kondo effect with ultracold atoms. Our system consists of a Fermi sea of spinless fermions interacting with an impurity atom of different species which is confined by an isotropic potential. The interspecies attraction can be tuned with an $s$-wave Feshbach resonance so that the impurity atom and a spinless fermion form a bound dimer that occupies a threefold-degenerate $p$ orbital of the confinement potential. Many-body scatterings of this dimer and surrounding spinless fermions occur with exchanging their angular momenta and thus exhibit the SU(3) orbital Kondo effect. The associated Kondo temperature has a universal leading exponent given by $T_K\propto\exp[-\pi/(3a_p k_F^3)]$ that depends only on an effective $p$-wave scattering volume $a_p$ and a Fermi wave vector $k_F$. We also elucidate a Kondo singlet formation at zero temperature and an anisotropic interdimer interaction mediated by surrounding spinless fermions. The Kondo effect thus realized in ultracold atom experiments may be observed as an increasing atom loss by lowering the temperature or with radio-frequency spectroscopy. Our scheme and its extension to a dense Kondo lattice will be useful to develop new insights into yet unresolved aspects of Kondo physics.