835 research outputs found

    Unimodality for free multiplicative convolution with free normal distributions on the unit circle

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    We study unimodality for free multiplicative convolution with free normal distributions {λt}t>0\{\lambda_t\}_{t>0} on the unit circle. We give four results on unimodality for μ⊠λt\mu\boxtimes\lambda_t: (1) if μ\mu is a symmetric unimodal distribution on the unit circle then so is μ⊠λt\mu\boxtimes \lambda_t at any time t>0t>0; (2) if μ\mu is a symmetric distribution on T\mathbb{T} supported on {eiθ:θ∈[−φ,φ]}\{e^{i\theta}: \theta \in [-\varphi,\varphi]\} for some φ∈(0,π/2)\varphi \in (0,\pi/2), then μ⊠λt\mu \boxtimes \lambda_t is unimodal for sufficiently large t>0t>0; (3) b⊠λt{\bf b} \boxtimes \lambda_t is not unimodal at any time t>0t>0, where b{\bf b} is the equally weighted Bernoulli distribution on {1,−1}\{1,-1\}; (4) λt\lambda_t is not freely strongly unimodal for sufficiently small t>0t>0. Moreover, we study unimodality for classical multiplicative convolution (with Poisson kernels), which is useful in proving the above four results.Comment: 19 pages, 4 figure

    Can Spinor Dipolar Effects be Observed in Bose-Einstein Condensates?

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    Weak dipolar effects in atomic Bose-Einstein condensates (BECs) have recently been predicted to develop spin textures. However, observation of these effects requires magnetic field as low as ∼10μ\sim 10 \muG for spin-1 alkali BECs, so that they are not washed out by the Zeeman effect. We present a scheme to observe the magnetic dipole-dipole interaction in alkali BECs under a realistic magnetic field of ∼100\sim 100 mG. Our scheme enables us to extract genuine dipolar effects and should apply also to 52^{52}Cr BECs.Comment: 4 pages, 3 figure

    Breaking of Chiral Symmetry and Spontaneous Rotation in a Spinor Bose-Einstein Condensate

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    We show that a spin-1 Bose-Einstein condensate with ferromagnetic interactions spontaneously generates a topological spin texture, in which the m = \pm 1 components of the magnetic sublevels form vortices with opposite circulations. This phenomenon originates from an interplay between ferromagnetic interactions and spin conservation.Comment: 5 pages, 4 figure
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