Higgs mode in a strongly interacting fermionic superfluid

TL;DR

This paper reports the experimental observation of the Higgs mode in a strongly-interacting fermionic superfluid, demonstrating its stability and eventual decay as interactions become very strong, thus advancing understanding of collective excitations in correlated systems.

Contribution

First direct observation of the Higgs mode in a strongly-interacting superfluid Fermi gas, showing its behavior and stability limits in such systems.

Findings

Higgs mode observed at frequency 2Δ/h with periodic modulation

Mode broadens and disappears as coupling strength increases

Signatures of Higgs mode instability when Cooper pairs form tightly bound dimers

Abstract

Higgs and Goldstone modes are possible collective modes of an order parameter upon spontaneously breaking a continuous symmetry. Whereas the low-energy Goldstone (phase) mode is always stable, additional symmetries are required to prevent the Higgs (amplitude) mode from rapidly decaying into low-energy excitations. In high-energy physics, where the Higgs boson has been found after a decades-long search, the stability is ensured by Lorentz invariance. In the realm of condensed--matter physics, particle--hole symmetry can play this role and a Higgs mode has been observed in weakly-interacting superconductors. However, whether the Higgs mode is also stable for strongly-correlated superconductors in which particle--hole symmetry is not precisely fulfilled or whether this mode becomes overdamped has been subject of numerous discussions. Experimental evidence is still lacking, in particular owing to the difficulty to excite the Higgs mode directly. Here, we observe the Higgs mode in a strongly-interacting superfluid Fermi gas. By inducing a periodic modulation of the amplitude of the superconducting order parameter $\Delta$, we observe an excitation resonance at frequency $2\Delta/h$. For strong coupling, the peak width broadens and eventually the mode disappears when the Cooper pairs turn into tightly bound dimers signalling the eventual instability of the Higgs mode.