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Anisotropic Superfluid Behavior of a Dipolar Bose-Einstein Condensate

Matthias Wenzel, Fabian Böttcher, Jan-Niklas Schmidt, Michael Eisenmann, Tim Langen, Tilman Pfau, and Igor Ferrier-Barbut
Phys. Rev. Lett. 121, 030401 – Published 17 July 2018
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Abstract

We present transport measurements on a dipolar superfluid using a Bose-Einstein condensate of Dy162 with strong magnetic dipole-dipole interactions. By moving an attractive laser beam through the condensate we observe an anisotropy in superfluid flow. This observation is compatible with an anisotropic critical velocity for the breakdown of dissipationless flow, which, in the spirit of the Landau criterion, can directly be connected to the anisotropy of the underlying dipolar excitation spectrum. In addition, the heating rate above this critical velocity reflects the same anisotropy. Our observations are in excellent agreement with simulations based on the Gross-Pitaevskii equation and highlight the effect of dipolar interactions on macroscopic transport properties, rendering dissipation anisotropic.

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  • Received 12 April 2018

DOI:https://doi.org/10.1103/PhysRevLett.121.030401

© 2018 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied PhysicsAtomic, Molecular & Optical

Authors & Affiliations

Matthias Wenzel, Fabian Böttcher, Jan-Niklas Schmidt, Michael Eisenmann, Tim Langen, Tilman Pfau, and Igor Ferrier-Barbut*

  • 5. Physikalisches Institut and Center for Integrated Quantum Science and Technology (IQST), Universität Stuttgart, Pfaffenwaldring 57, 70569 Stuttgart, Germany

  • *i.ferrier-barbut@physik.uni-stuttgart.de

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Issue

Vol. 121, Iss. 3 — 20 July 2018

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Images

  • Figure 1
    Figure 1

    Probing anisotropic critical velocity. (a) Excitation spectrum of a homogeneous dipolar Bose gas. The speed of sound vs depends on the direction of the excitation k with respect to the dipole polarization B, denoted by the angle α. (b) The critical velocity vc (solid), as given by Eq. (2), becomes anisotropic and is in general lower than vs (dashed). (c) Schematic of the experiment. We drag an attractive laser beam through a dipolar condensate perpendicular (α=90°, blue) and parallel (α=0°, red) to the magnetic field direction.

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  • Figure 2
    Figure 2

    Temperature of the dBEC after stirring for (a) the isotropic case with Bz^ and (b) the anisotropic case with Bx^ in an almost cylindrical trap. In (c) the trap is additionally reshaped to invert the cloud aspect ratio. The stirring beam is moved along the x (red squares) or y (blue circles) axis, as illustrated in the insets with example in situ images. Critical velocities are extracted by a linear fit (dashed) and marked with arrows. In (a) the response is isotropic with vx=0.20(5) and vy=0.20(7)mm/s, while we observe a clear difference in (b) with v=0.16(2)mm/s along y^ and v=0.36(3)mm/s along x^. In (c) we extract v=0.12(3) and v=0.26(4)mm/s proving that the observed anisotropy remains even when inverting the anisotropy of the atomic cloud. Data points with stirring frequency matching the trapping frequencies (gray) are excluded from the analysis. Simulations of the eGPE for a single stirring cycle (solid lines) show excellent agreement with the experiment. See text for further parameters.

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