Measurement of the superfluid fraction of a supersolid by Josephson effect.
basic_science · Level V
Where this comes from
- Record sourced from PubMed, PMID 38720083.
- Also identified by DOI 10.1038/s41586-024-07361-9 and PMC identifier 11111407.
- Licence recorded as CC BY.
- The licence permits redistribution, so the abstract is shown in full and the full text is available from the publisher.
Abstract
A new class of superfluids and superconductors with spatially periodic modulation of the superfluid density is arising<sup>1-12</sup>. It might be related to the supersolid phase of matter, in which the spontaneous breaking of gauge and translational symmetries leads to a spatially modulated macroscopic wavefunction<sup>13-16</sup>. This relation was recognized only in some cases<sup>1,2,5-9</sup> and there is the need for a universal property quantifying the differences between supersolids and ordinary matter, such as the superfluid fraction, which measures the reduction in superfluid stiffness resulting from the spatial modulation<sup>16-18</sup>. The superfluid fraction was introduced long ago<sup>16</sup>, but it has not yet been assessed experimentally. Here we demonstrate an innovative method to measure the superfluid fraction based on the Josephson effect, a ubiquitous phenomenon associated with the presence of a physical barrier between two superfluids or superconductors<sup>19</sup>, which might also be expected for supersolids<sup>20</sup>, owing to the spatial modulation. We demonstrate that individual cells of a supersolid can sustain Josephson oscillations and we show that, from the current-phase dynamics, we can derive directly the superfluid fraction. Our study of a cold-atom dipolar supersolid<sup>7</sup> reveals a relatively large sub-unity superfluid fraction that makes realistic the study of previously unknown phenomena such as partially quantized vortices and supercurrents<sup>16-18</sup>. Our results open a new direction of research that may unify the description of all supersolid-like systems.