Barnett Ryan, Turner Ari, Demler Eugene
Department of Physics, Harvard University, Cambridge, Massachusetts 02138, USA.
Phys Rev Lett. 2006 Nov 3;97(18):180412. doi: 10.1103/PhysRevLett.97.180412.
We consider many-body states of bosonic spinor atoms which, at the mean-field level, can be characterized by a single-particle wave function for the Bose-Einstein condensation and Mott insulating states. We describe and apply a classification scheme that makes explicit the spin symmetries of such states and enables one to naturally analyze their collective modes and topological excitations. Quite generally, the method allows classification of a spin F system as a polyhedron with 2F vertices. We apply the method to the many-body states of bosons with spins two and three. For spin-two atoms we find the ferromagnetic state, a continuum of nematic states, and a state having the symmetry of the point group of the regular tetrahedron. For spin-three atoms we obtain similar ferromagnetic and nematic phases as well as states having symmetries of various types of polyhedra with six vertices.
我们考虑玻色子自旋原子的多体状态,在平均场水平下,这些状态可以由玻色 - 爱因斯坦凝聚态和莫特绝缘态的单粒子波函数来表征。我们描述并应用一种分类方案,该方案明确了此类状态的自旋对称性,并使人们能够自然地分析它们的集体模式和拓扑激发。一般来说,该方法允许将自旋为F的系统分类为具有2F个顶点的多面体。我们将该方法应用于自旋为二和三的玻色子的多体状态。对于自旋为二的原子,我们发现了铁磁态、连续的向列相态以及具有正四面体点群对称性的状态。对于自旋为三的原子,我们得到了类似的铁磁相和向列相以及具有六个顶点的各种类型多面体对称性的状态。