Abstract

We investigate the stability of vortices in two-dimensional Bose--Einstein condensates. In analogy with rotating spacetimes and with a careful account of boundary conditions, we show that the dynamical instability of multiply quantized vortices in trapped condensates persists in untrapped, spatially homogeneous geometries and has an ergoregion nature with some modification due to the peculiar dispersion of Bogoliubov sound. Our results open new perspectives to the physics of vortices in trapped condensates, where multiply quantized vortices can be stabilized by interference effects and singly charged vortices can become unstable in suitably designed trap potentials. We show how superradiant scattering can be observed also in the short-time dynamics of dynamically unstable systems, providing an alternative point of view on dynamical (in)stability phenomena in spatially finite systems.

Highlights

  • Quantized vortices are one of the key features of superfluids and Bose–Einstein condensates (BECs) and have received a great deal of attention in the last decades, both theoretically and experimentally [1,2]

  • Quite recently, convincing evidence that doubly quantized vortex are unstable in a spatially uniform BEC was reported [11], while dynamical stability of such configurations had been previously claimed by several authors [7,12]

  • An interesting way to look at this paradigmatic problem of condensed-matter physics is the one offered by analog gravity [13], which relies on the fact that collective excitation modes on top of a moving medium are described by the same equations as a massless scalar field on a curved space-time

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Summary

INTRODUCTION

Quantized vortices are one of the key features of superfluids and Bose–Einstein condensates (BECs) and have received a great deal of attention in the last decades, both theoretically and experimentally [1,2]. We are here interested in quantized vortices in superfluids: their purely azimuthal vθ ∝ 1/r irrotational flow pattern becomes supersonic in the vicinity of the vortex core and corresponds to an analog rotating space-time with an ergoregion but no horizon. This naturally suggests the possibility of observing ergoregion instabilities in infinite condensates. Application of our formalism to singly quantized vortices brings the unexpected consequence that their celebrated dynamical stability is not a general fact, but a consequence of the spatially homogeneous or harmonic trap geometries usually considered in the literature: more complex configurations showing an inner density bump followed by a constant density plateau turn out to be dynamically unstable against the vortex spiralling out, even at zero temperature.

VORTICES AND THE LINEAR PROBLEM
VORTICES IN TRAPPED BECS
A CHARGE 2 VORTEX IN AN INFINITE BEC
Outgoing boundary conditions
HIGHER CHARGE VORTICES
ON THE STABILITY OF SINGLY CHARGED VORTICES
A TIME-DEPENDENT PERSPECTIVE
VIII. CONCLUSIONS
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