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Observation of cooperative Mie scattering from an ultracold atomic cloud

Source: Phys. Rev. A 82, 011404 (2010); doi:10.1103/PhysRevA.82.011404

Published 26 July 2010

PACS
  • 37.10.Vz
    Mechanical effects of light on atoms, molecules and ions
  • 42.50.Ct
    Quantum description of interaction of light and matter; related experiments
  • 42.25.Fx
    Optical diffraction and scattering
  • 32.80.Qk
    Coherent control of atomic interactions with photons
  • YEAR: 2010
PUBLICATION DATA
ISSN:
1553-9601 (online)
Publisher:
AIP is a member of CrossRef APS
H. Bender,1 C. Stehle,1 S. Slama,1 R. Kaiser,3 N. Piovella,2 C. Zimmermann,1 and Ph. W. Courteille1,3,4
1Physikalisches Institut, Eberhardt-Karls-Universität Tübingen, D-72076 Tübingen, Germany
2Dipartimento di Fisica, Università Degli Studi di Milano, Via Celoria 16, I-20133 Milano, Italy
3Institut Non Linéaire de Nice, CNRS, Université de Nice Sophia-Antipolis, F-06560 Valbonne, France
4Instituto de Física de São Carlos, Universidade de São Paulo, 13560-970 São Carlos, SP, Brazil

Scattering of light at a distribution of scatterers is an intrinsically cooperative process, which means that the scattering rate and the angular distribution of the scattered light are essentially governed by bulk properties of the distribution, such as its size, shape, and density, although local disorder and density fluctuations may have an important impact on the cooperativity. Via measurements of the radiation pressure force exerted by a far-detuned laser beam on a very small and dense cloud of ultracold atoms, we are able to identify the respective roles of superradiant acceleration of the scattering rate and of Mie scattering in the cooperative process. They lead, respectively, to a suppression or an enhancement of the radiation pressure force. We observe a maximum in the radiation pressure force as a function of the phase shift induced in the incident laser beam by the cloud's refractive index. The maximum marks the borderline of the validity of the Rayleigh-Debye-Gans approximation from a regime, where Mie scattering is more complex. Our observations thus help to clarify the intricate relationship between Rayleigh scattering of light at a coarse-grained ensemble of individual scatterers and Mie scattering at the bulk density distribution. ©2010 The American Physical Society
History: Received 28 April 2010; published 26 July 2010
Permalink: http://link.aps.org/abstract/PRA/v82/e011404
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