Abstract

We theoretically investigate a supersymmetric collective mode called Goldstino in a Bose-Fermi mixture. The explicit supersymmetry breaking, which is unavoidable in cold atom experiments, is considered. We derive the Gell-Mann--Oakes-Renner (GOR) relation for the Goldstino, which gives the relation between the energy gap at the zero momentum and the explicit breaking term. We also numerically evaluate the gap of Goldstino above the Bose-Einstein condensation temperature within the random phase approximation (RPA). While the gap obtained from the GOR relation coincides with that in the RPA for the mass-balanced system, there is a deviation from the GOR relation in the mass-imbalanced system. We point out the deviation becomes large when the Goldstino pole is close to the branch point, although it is parametrically a higher order with respect to the mass-imbalanced parameter. To examine the existence of the goldstino pole in realistic cold atomic systems, we show how the mass-imbalance effect appears in $^6$Li-$^7$Li, $^{40}$K-$^{41}$K, and $^{173}$Yb-$^{174}$Yb mixtures. Furthermore, we analyze the Goldstino spectral weight in a $^{173}$Yb-$^{174}$Yb mixture with realistic interactions and show a clear peak due to the Goldstino pole. As a possibility to observe the Goldstino spectrum in cold atom experiments, we discuss the effects of the Goldstino pole on the fermionic single-particle excitation as well as the relationship between the GOR relation and Tan's contact.

Highlights

  • Supersymmetry is symmetry with respect to an interchange between bosons and fermions [1,2,3]

  • We have theoretically investigated the gapped Goldstino mode in an ultracold atomic Bose-Fermi mixture with explicitly broken supersymmetry

  • We calculate the Goldstino gap at the first order of the explicit symmetry breaking and compare it with the numerical results obtained within the random phase approximation (RPA)

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Summary

INTRODUCTION

Supersymmetry is symmetry with respect to an interchange between bosons and fermions [1,2,3]. Explicit supersymmetry breaking such as the mass imbalance between fermions and bosons is unavoidable in cold-atom experiments In this case, the Goldstino has a finite energy gap associated with the explicit breaking parameters. By developing a gap formula for the Goldstino, which corresponds to the Gell-Mann–Oakes–Renner (GOR) relation in quantum chromodynamics [39], based on the memory function formalism [40], we show how the explicit supersymmetry-breaking terms affect the Goldstino gap in these systems By comparing it with the numerical results of the random phase approximation (RPA), we clarify that the effects of the branch point are significant in the presence of the mass imbalance between fermions and bosons. We discuss how to observe the Goldstino gap from the single-particle spectral function of a Fermi atom. In Appendix C, we discuss the cutoff dependence of the fermionic single-particle spectral function

FORMALISM
Gell-Mann–Oakes–Renner relation
Mean-field approximation
Random phase approximation
Thermodynamic quantities
Spectral properties of the Goldstino
FERMIONIC SINGLE-PARTICLE SPECTRUM
SUMMARY
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