Second sound and the superfluid fraction in a resonantly interacting Fermi gas

TL;DR

This paper reports the first observation of second sound in an ultracold Fermi gas, providing a new way to measure the superfluid fraction and explore superfluid properties in strongly interacting quantum gases.

Contribution

It demonstrates the detection of second sound in a resonantly interacting Fermi gas, enabling direct measurement of the superfluid fraction's temperature dependence.

Findings

First observation of second sound in ultracold Fermi gas

Superfluid fraction's temperature dependence measured

Validates two-fluid model in quantum gases

Abstract

Superfluidity is a macroscopic quantum phenomenon, which shows up below a critical temperature and leads to a peculiar behavior of matter, with frictionless flow, the formation of quantized vortices, and the quenching of the moment of inertia being intriguing examples. A remarkable explanation for many phenomena exhibited by a superfluid at finite temperature can be given in terms of a two-fluid mixture comprised of a normal component that behaves like a usual fluid and a superfluid component with zero viscosity and zero entropy. Important examples of superfluid systems are liquid helium and neutron stars. More recently, ultracold atomic gases have emerged as new superfluid systems with unprecedented possibilities to control interactions and external confinement. Here we report the first observation of `second sound' in an ultracold Fermi gas with resonant interactions. Second sound is a striking manifestation of the two-component nature of a superfluid and corresponds to an entropy wave, where the superfluid and the non-superfluid components oscillate in opposite phase, different from ordinary sound (`first sound'), where they oscillate in phase. The speed of second sound depends explicitly on the value of the superfluid fraction, a quantity sensitive to the spectrum of elementary excitations. Our measurements allow us to extract the temperature dependence of the superfluid fraction, which in strongly interacting quantum gases has been an inaccessible quantity so far.