2006
DOI: 10.1103/physrevb.74.155124
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Biaxial spin-nematic phase of two-dimensional disordered rotor models andS=1bosons in optical lattices

Abstract: We show that the ground state of disordered rotor models with quadrupolar interactions can exhibit biaxial nematic ordering in the disorder-averaged sense. We present a mean-field analysis of the model and demonstrate that the biaxial phase is stable against small quantum fluctuations. We point out the possibility of experimental realization of such rotor models using ultracold spin-one Bose atoms in a spin-dependent and disordered optical lattice in the limit of a large number of atoms per site and also sugge… Show more

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Cited by 9 publications
(7 citation statements)
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“…Although we set U 2 /U 0 optimal values for validity of the theory that is not realistic in the present experimental status, the obtained results may be applicable to 23 Na with U 2 /U 0 = 0.04. The first-order phase transition dominates the larger part of the phase boundary and the region of the metastable SF phase in the phase diagram gets larger for smaller U 2 /U 0 [14,17].…”
Section: Discussionmentioning
confidence: 95%
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“…Although we set U 2 /U 0 optimal values for validity of the theory that is not realistic in the present experimental status, the obtained results may be applicable to 23 Na with U 2 /U 0 = 0.04. The first-order phase transition dominates the larger part of the phase boundary and the region of the metastable SF phase in the phase diagram gets larger for smaller U 2 /U 0 [14,17].…”
Section: Discussionmentioning
confidence: 95%
“…The first-order phase transition dominates the larger part of the phase boundary and the region of the metastable SF phase in the phase diagram gets larger for smaller U 2 /U 0 [14,17]. The effect of the first-order phase transition, therefore, may be remarkable and easy to study experimentally for 23 Na.…”
Section: Discussionmentioning
confidence: 99%
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“…With spin-dependent OLs, atomic internal degrees of freedom such as its spin or pseudo-spin (group of internal states), are coupled to its spatial degrees of freedom. This can give rise to interesting phenomena [9][10][11][12][13][14][15][16][17][18] absent in spin-independent lattices. For example, attractive Fermi gases in 1D lattices support three-body bound states with only two-body interactions when the tunneling rates are spin-dependent [19].…”
Section: Introductionmentioning
confidence: 99%