43rd Annual Meeting of the APS Division of Atomic, Molecular and Optical Physics
Volume 57, Number 5
Monday–Friday, June 4–8, 2012;
Orange County, California
Session C1: Invited Session: Dipolar Quantum Gases
2:00 PM–4:00 PM,
Tuesday, June 5, 2012
Room: Grand Ballroom BCD
Chair: Doerte Blume, Washington State University
Abstract ID: BAPS.2012.DAMOP.C1.2
Abstract: C1.00002 : Dipolar Chromium BECs
2:30 PM–3:00 PM
Preview Abstract
Abstract
Author:
Bruno Laburthe-Tolra
(CNRS)
Bose-Einstein condensates (BECs) made of 52Cr atoms reveal new phenomena,
due to the presence of the long-range and anisotropic dipole-dipole
interactions (see for example [1]).
In this talk, I will describe the effect of dipolar interactions on the
properties of multi-component (spinor) Cr condensates at extremely low
magnetic fields. Due to its anisotropy, the dipolar interaction introduces
magnetization-changing collisions, which dynamically frees the magnetization
of the gas. We have thus observed a demagnetization of the BEC when the
magnetic field is quenched below a critical value Bc corresponding to a
phase transition between a ferromagnetic and a non-polarized ground state.
The phase transition is due to an inter-play between spin-dependent
interactions and the linear Zeeman effect [2]. We have also studied the
thermodynamic properties of spinor Cr atoms, and we have observed that above
the critical field Bc, the ferromagnetic nature of BECs leads to the
spontaneous magnetization of the cloud when BEC is reached [3].
I will also describe the control of magnetization-changing collisions in
optical lattices. We investigate a scheme in which dipolar relaxation is
resonant when the energy released in dipolar relaxation matches a band
excitation resonance [4]. This scheme, which may produce correlated pairs of
rotating states in each lattice site, can be viewed as the equivalent of the
Einstein-de-Haas effect. Although rotation is not yet produced in our
experiment, I will present first experimental results of these dipolar
resonances, which show a pronounced anisotropic behaviour.
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[1] T. Lahaye et al., Rep. Prog. Phys. 72, 126401 (2009), G. Bismut, et al.,
Phys. Rev. Lett. 105, 040404 (2010)
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[2] B. Pasquiou et al., Phys. Rev. Lett. 106, 255303 (2011)
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[3] B. Pasquiou, arXiv:1110.0786, to be published in Phys. Rev. Lett. (2012)
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[4] B. Pasquiou et al., Phys. Rev. Lett. 106, 015301 (2011)
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2012.DAMOP.C1.2