Theory of Radio Frequency Spectroscopy Experiments in Ultracold Fermi Gases and Their Relation to Photoemission Experiments in the Cuprates

TL;DR

This paper reviews RF spectroscopy in ultracold Fermi gases, connecting experimental and theoretical insights with photoemission studies in cuprates, highlighting the BCS-BEC crossover and potential for future research.

Contribution

It provides a systematic overview of RF spectroscopy theory and its relation to cuprate photoemission, suggesting new research directions in cold gases for condensed matter insights.

Findings

RF spectroscopy can be described within the BCS-Leggett framework.

The theory captures key phenomena observed in experiments.

Cold Fermi gases can model aspects of cuprate superconductors.

Abstract

In this paper we present an overview of radio frequency (RF) spectroscopy in the atomic Fermi superfluids. An ultimate goal is to suggest new directions in the cold gas research agenda from the condensed matter perspective.Our focus is on the experimental and theoretical literature of cold gases and photoemission spectroscopy of the cuprates particularly as it pertains to areas of overlap. This paper contains a systematic overview of the theory of RF spectroscopy, both momentum integrated and momentum resolved. We discuss the effects of traps, population imbalance, final state interactions over the entire range of temperatures and compare theory and experiment. We show that this broad range of phenomena can be accomodated within the BCS-Leggett description of BCS-BEC crossover and that this scheme also captures some of the central observations in photoemission experiments in the cuprates. In this last context, we note that the key themes which have emerged in cuprate photoemission studies involve characterization of the fermionic self energy, of the pseudogap and of the effects of superconducting coherence (in passing from above to below the superfluid transition temperature, $T_c$).These issues have a counterpart in the cold Fermi gases and it would be most useful in future to use these atomic systems to address these and the more sweeping question of how to describe that anomalous superfluid phase which forms in the presence of a normal state excitation gap.