LPTMS, CNRS, Univ. Paris-Sud, Université Paris-Saclay, 91405 Orsay, France.
Centre de Physique Théorique, Ecole Polytechnique, CNRS, Université Paris-Saclay, F-91128 Palaiseau, France.
Phys Rev Lett. 2018 Apr 13;120(15):157201. doi: 10.1103/PhysRevLett.120.157201.
Recently, the frustrated XY model for spins 1/2 on the honeycomb lattice has attracted a lot of attention in relation with the possibility to realize a chiral spin liquid state. This model is relevant to the physics of some quantum magnets. Using the flexibility of ultracold atom setups, we propose an alternative way to realize this model through the Mott regime of the bosonic Kane-Mele-Hubbard model. The phase diagram of this model is derived using bosonic dynamical mean-field theory. Focusing on the Mott phase, we investigate its magnetic properties as a function of frustration. We do find an emergent chiral spin state in the intermediate frustration regime. Using exact diagonalization we study more closely the physics of the effective frustrated XY model and the properties of the chiral spin state. This gapped phase displays a chiral order, breaking time-reversal and parity symmetry, but is not topologically ordered (the Chern number is zero).
最近,在与实现手性自旋液体态的可能性有关的情况下,蜂窝晶格上的受挫 XY 模型吸引了很多关注。这个模型与一些量子磁体的物理性质有关。利用超冷原子装置的灵活性,我们提出了一种通过玻色 Kane-Mele-Hubbard 模型的莫特区来实现这个模型的替代方法。通过玻色动力学平均场理论,推导出这个模型的相图。关注莫特相,我们研究了其作为受挫函数的磁性质。我们确实在中间受挫区域发现了一种新兴的手性自旋态。使用精确对角化,我们更仔细地研究了有效受挫 XY 模型的物理性质和手性自旋态的性质。这个带隙相显示出手性序,破坏时间反转和宇称对称性,但不是拓扑有序的(Chern 数为零)。