Two-dimensional superfluidity and quantum turbulence are directly connected to the microscopic dynamics of quantized vortices. However, surface effects have prevented direct observations of coherent vortex dynamics in strongly-interacting two-dimensional systems. Here, we overcome this challenge by confining a twodimensional droplet of superfluid helium at microscale on the atomically-smooth surface of a silicon chip. An on-chip optical microcavity allows laser-initiation of vortex clusters and nondestructive observation of their decay in a single shot. Coherent dynamics dominate, with thermal vortex diffusion suppressed by six orders-of-magnitude. This establishes a new on-chip platform to study emergent phenomena in strongly-interacting superfluids, test astrophysical dynamics such as those in the superfluid core of neutron stars in the laboratory, and construct quantum technologies such as precision inertial sensors.
arXiv:1902.04409v1 [cond-mat.other] 7 Feb 2019Strongly-interacting many-body quantum systems exhibit rich behaviours of significance to areas ranging from superconductivity [1] to quantum computation [2, 3], astrophysics [4][5][6], and even string theory [7]. The first example of such a behaviour, superfluidity, was discovered more than eighty years ago in cryogenically cooled liquid helium-4 [8]. Quite remarkably, it was found to persist even in thin two-dimensional films [9], for which the well-known Mermin-Wagner theorem precludes condensation into a superfluid phase in the thermodynamic limit [10]. This apparent contradiction was resolved by Berezinskii, Kosterlitz and Thouless (BKT), who predicted that quantized vortices allow a topological phase transition into superfluidity [11,12]. It is now recognized that quantized vortices also dominate much of the out-of-equilibrium dynamics of two-dimensional superfluids, such as quantum turbulence [13].Recently, laser control and imaging of vortices in ultracold gases [14, 15] and semiconductor exciton-polariton systems [16,17] has provided rich capabilities to study superfluid dynamics [18] including, for example, the formation of collective vortex dipoles with negative temperature and large-scale order [19, 20] as predicted by Lars Onsager seventy years ago [21]. However, these experiments are generally limited to the regime of weak interactions, where the Gross-Pitaevskii equation provides a microscopic model of the dynamics of the superfluid. The regime of strong interactions can be reached by tuning the atomic scattering length in ultracold gases [22, 23]. However, technical challenges have limited investigations of nonequilibrium phenomena [22]. The strongly-interacting regime defies a microscopic theoretical treatment and is the relevant regime for superfluid helium as well as for astrophysical superfluid phenomena such as pulsar glitches [24] and superfluidity of the quark-gluon plasma in the early universe [6]. The vortex dynamics in this regime are typically predicted using phenomenological vortex models. However, whether the vortices...