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Collision of two spin-polarized fermionic clouds

O. Goulko, F. Chevy, and C. Lobo
Phys. Rev. A 84, 051605(R) – Published 28 November 2011
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Abstract

We study the collision of two spin-polarized Fermi clouds in a harmonic trap using a simulation of the Boltzmann equation. As observed in recent experiments, we find three distinct regimes of behavior. For weak interactions the clouds pass through each other. If interactions are increased they approach each other exponentially and for strong interactions they bounce off each other several times. We thereby demonstrate that all these phenomena can be reproduced using a semiclassical collisional approach and that these changes in behavior are associated with an increasing collision rate. We then show that the oscillation of the clouds in the bounce regime is an example of an unusual case in quantum gases: a nonlinear coupling between collective modes, namely, the spin dipole mode and the axial breathing mode, which is enforced by collisions. We also determine the frequency of the bounce as a function of the final temperature of the equilibrated system.

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  • Received 29 June 2011

DOI:https://doi.org/10.1103/PhysRevA.84.051605

©2011 American Physical Society

Authors & Affiliations

O. Goulko1,*, F. Chevy2, and C. Lobo3

  • 1Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Centre for Mathematical Sciences, Cambridge CB3 0WA, United Kingdom
  • 2Laboratoire Kastler Brossel, Ecole Normale Supérieure, 24 rue Lhomond, F-75231 Paris Cedex 05, France
  • 3School of Mathematics, University of Southampton, Highfield, Southampton SO17 1BJ, United Kingdom

  • *o.goulko@damtp.cam.ac.uk

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Issue

Vol. 84, Iss. 5 — November 2011

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Images

  • Figure 1
    Figure 1
    Bottom panel: The normalized dipole mode d(t)/d0 (solid lines) and breathing mode b(t)/b (dashed lines) for the three different behaviors: transmission (left), intermediate (middle), and bounce (right). Top panel: The corresponding collision rate per particle γ/ωz measured in the region with |z|σz/2 around the trap center, where σz=Tinit/mωz2.Reuse & Permissions
  • Figure 2
    Figure 2
    The transition between bounce and intermediate regimes (filled symbols, the lines to guide the eye) and between intermediate and transmission regimes (open symbols). The red circles correspond to d0=43.1lz, the blue triangles to d0=64.6lz and the green squares to d0=129.3lz, where lz=1/mωz. It is clearly visible that the intermediate-transmission transition is independent of d0. The dashed line corresponds to constant relaxation time 1/τdip=1.83ωz.Reuse & Permissions
  • Figure 3
    Figure 3
    The frequency ω/ωz of the dipole mode d(t) (red circles) and the breathing mode b(t) (blue triangles) vs the final temperature for |k̃Fa|=1. All data were obtained for equal initial temperature Tinit=0.4T̃F by varying d0. The solid line is the prediction from Ref. [17].Reuse & Permissions
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