Atom Loss Resonances in a Bose-Einstein Condensate

Christian Langmack, D. Hudson Smith, and Eric Braaten
Phys. Rev. Lett. 111, 023003 – Published 9 July 2013
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Abstract

Atom loss resonances in ultracold trapped atoms have been observed at scattering lengths near atom-dimer resonances, at which Efimov trimers cross the atom-dimer threshold, and near two-dimer resonances, at which universal tetramers cross the dimer-dimer threshold. We propose a new mechanism for these loss resonances in a Bose-Einstein condensate of atoms. As the scattering length is ramped to the large final value at which the atom loss rate is measured, the time-dependent scattering length generates a small condensate of shallow dimers coherently from the atom condensate. The coexisting atom and dimer condensates can be described by a low-energy effective field theory with universal coefficients that are determined by matching exact results from few-body physics. The classical field equations for the atom and dimer condensates predict narrow enhancements in the atom loss rate near atom-dimer resonances and near two-dimer resonances due to inelastic dimer collisions.

  • Figure
  • Received 24 February 2013

DOI:https://doi.org/10.1103/PhysRevLett.111.023003

© 2013 American Physical Society

Authors & Affiliations

Christian Langmack, D. Hudson Smith, and Eric Braaten

  • Department of Physics, The Ohio State University, Columbus, Ohio 43210, USA

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Issue

Vol. 111, Iss. 2 — 12 July 2013

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