2010
DOI: 10.1103/physrevb.81.184526
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Low-energy dynamics of spinor condensates

Abstract: We present a derivation of the low energy Lagrangian governing the dynamics of the spin degrees of freedom in a spinor Bose condensate, for any phase in which the average magnetization vanishes. This includes all phases found within mean-field treatments except for the ferromagnet, for which the low energy dynamics has been discussed previously. The Lagrangian takes the form of a sigma model for the rotation matrix describing the local orientation of the spin state of the gas.

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Cited by 40 publications
(33 citation statements)
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“…In particular, it has led to the demonstration that, in the superfluid phase of spin-1 bosons on a lattice, the SU(2) symmetry is spontaneously broken, by contrast to the case of bosons in a single mode, which require an SU(2) symmetry-breaking interaction to build a polar condensate. It will be very interesting to investigate the implications of this result on the dynamics of spinor condensates [34] in the presence of a lattice.…”
Section: Introductionmentioning
confidence: 96%
“…In particular, it has led to the demonstration that, in the superfluid phase of spin-1 bosons on a lattice, the SU(2) symmetry is spontaneously broken, by contrast to the case of bosons in a single mode, which require an SU(2) symmetry-breaking interaction to build a polar condensate. It will be very interesting to investigate the implications of this result on the dynamics of spinor condensates [34] in the presence of a lattice.…”
Section: Introductionmentioning
confidence: 96%
“…However, the Berkeley experiment [16] shows that the magnetization is not fully polarized over the entire condensate. Meanwhile, the Majorana representation has been employed to describe general spin states [23,24]. Barnett et.…”
Section: Introductionmentioning
confidence: 99%
“…al. [23] have developed the mean-field hydrodynamic equations that involve the Landau-Lifshitz equations for the spin-node vectors and reproduce collective excitations from the viewpoint of the point-group symmetry, while Lamacraft [24] has derived the low-energy Lagrangian and obtained the spin-wave spectra. In this paper, we derive the most general mean-field hydrodynamic equations for spin-1 BECs that are equivalent to the multi-component GP equations and expressed in terms of observable quantities such as the magnetization vector and the nematic (or quadrupolar) tensor.…”
Section: Introductionmentioning
confidence: 99%
“…To gain further insight, we express each <J>(L) in Majorana representation as a set of 2L points (referred to as Majorana points) on the unit sphere S2 [11,[13][14][15], To accomplish it, we use the Schwinger bosons representation of angular momentum states,…”
Section: M=-lmentioning
confidence: 99%