Abstract

The phenomenon of superfluidity in open Bose–Einstein condensates (BEC) is analysed numerically and analytically. It is found that a superfluid phase is feasible above the speed of sound, when forces due to inhomogeneous non-equilibrium processes oppose the contributions of homogeneous processes. Furthermore a regime of accelerating impurities can be observed for particular pumping/decay strategies. All findings are derived within the complex Gross–Pitaevskii (GP) theory extended to include creation and annihilation terms. Utilising this framework the effective force acting on an impurity as it moves with velocity v through the open condensate can be calculated. The result shows that the drag force is continuously increasing with increasing velocity starting from the state of zero motion at v = 0, a property that can be traced down to the additional homogeneous annihilation/creation term in the extended GP model. For very large velocities however we observe a reversion of the drag force. Our findings stand in stark contrast to the concept of a topological phase transition to frictionless flow below a critical velocity as observed for equilibrium BEC analytically (Astrakharchik and Pitaevskii 2004 Phys. Rev. A 70 013608; Pinsker 2017 Physica B 521 36–42), numerically (Winiecki et al 1999 Phys. Rev. Lett. 82 26) and for trapped atoms experimentally (Desbuquois et al 2012 Nat. Phys. 8 645; Zwierlein et al 2006 Nature 442 54–58).

Highlights

  • What defines superfluidity of a many-body system? The answer can be given in terms of a statement based on Landau’s theory of superfluidity [1,2,3]: below a certain critical velocity, due to non-existing energetically affordable elementary excitations within the many-body quantum system, an impurity moves dissipationless through the superfluid state of matter

  • It is found that a superfluid phase is feasible above the speed of sound, when forces work may be used under the terms of the Creative due to inhomogeneous non-equilibrium processes oppose the contributions of homogeneous

  • For contrasting observations on the equilibrium case we refer to [6], where the classical superfluid regime is discussed for extended impurities and we note the work discussing homogeneous pumping where no acceleration has been observed, which is consistent with the results presented here [63] as key to impurity acceleration is sculpting the density of the condensate wave function via inhomogeneous pumping processes as discussed here

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Summary

Introduction

What defines superfluidity of a many-body system? The answer can be given in terms of a statement based on Landau’s theory of superfluidity [1,2,3]: below a certain critical velocity, due to non-existing energetically affordable elementary excitations within the many-body quantum system, an impurity moves dissipationless through the superfluid state of matter. In figure 2(a) we numerically show the velocity dependence of the drag force acting on the Gaussian impurity in 2d for various pumping strengths, given a pump of the form

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