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Phys. Rev. B 80, 224502 (2009) [10 pages]

Magnetic phase diagram of a spin-1 condensate in two dimensions with dipole interaction

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Jonas A. Kjäll1, Andrew M. Essin1, and Joel E. Moore1,2
1Department of Physics, University of California, Berkeley, California 94720, USA
2Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA

Received 15 September 2009; revised 9 November 2009; published 8 December 2009

Several new features arise in the ground-state phase diagram of a spin-1 condensate trapped in an optical trap when the magnetic-dipole interaction between the atoms is taken into account along with confinement and spin precession. The boundaries between the regions of ferromagnetic and polar phases move as the dipole strength is varied and the ferromagnetic phases can be modulated. The magnetization of the ferromagnetic phase perpendicular to the field becomes modulated as a helix winding around the magnetic field direction with a wavelength inversely proportional to the dipole strength. This modulation should be observable for current experimental parameters in 87Rb. Hence the much-sought supersolid state with broken continuous translation invariance in one direction and broken global U(1) invariance, occurs generically as a metastable state in this system as a result of dipole interaction. The ferromagnetic state parallel to the applied magnetic field becomes striped in a finite system at strong dipolar coupling.

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.80.224502
DOI:
10.1103/PhysRevB.80.224502
PACS:
03.75.Kk, 03.75.Mn, 03.75.Lm