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F = 1 旋量玻色-爱因斯坦凝聚体的涡旋相图。

Vortex phase diagram of F=1 spinor Bose-Einstein condensates.

作者信息

Bulgakov Evgeny N, Sadreev Almas F

机构信息

Institute of Physics, Academy of Sciences, 660036 Krasnoyarsk, Russia.

出版信息

Phys Rev Lett. 2003 May 23;90(20):200401. doi: 10.1103/PhysRevLett.90.200401. Epub 2003 May 21.

Abstract

We have calculated the F=1 ground state of a spinor Bose-Einstein condensate trapped harmonic potential with an applied Ioffe-Pitchard magnetic field. The vortex phase diagram is found in the plane spanned by perpendicular and longitudinal magnetic fields. The ferromagnetic condensate has two vortex phases which differ by winding number in the spinor components. The two vortices for the F(z)=-1 antiferromagnetic condensate are separated in space. Moreover, we considered an average local spin |>| to testify to what extent it is parallel to magnetic field (the nonadiabatic effects). We have shown that the effects are important at vortex cores.

摘要

我们计算了在施加伊奥费-皮查德磁场的情况下,处于捕获谐波势中的自旋玻色-爱因斯坦凝聚体的F = 1基态。在由垂直和纵向磁场构成的平面中发现了涡旋相图。铁磁凝聚体有两个涡旋相,它们在自旋分量中的缠绕数不同。F(z)= -1反铁磁凝聚体的两个涡旋在空间中是分开的。此外,我们考虑了平均局部自旋|>|,以证明它在多大程度上与磁场平行(非绝热效应)。我们已经表明,这些效应在涡旋核心处很重要。

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