论文标题
Spin-1/2 Kitaev-Gamma链中的抗铁磁Kitaev点附近的经典自旋顺序
Classical spin order near antiferromagnetic Kitaev point in the spin-1/2 Kitaev-Gamma chain
论文作者
论文摘要
最近已经研究了一个最小的Kitaev-Gamma模型,以了解各种Kitaev系统。在一维的Kitaev-Gamma链中,使用非亚伯式玻璃体化和数值技术确定了出现的SU(2)$ _ 1 $相位和带有$ o_h \ rightArrow d_4 $对称破坏的等级1旋转订购相。然而,在有限伽玛相互作用的抗铁磁吉塔维亚区附近的难题仍未解决。在这里,我们关注此参数区域,并发现有两个新阶段,即,一个排名订购的阶段,具有$ o_h \ rightarrow d_3 $ symetry breaking,以及一个特殊的kitaev阶段。值得注意的是,$ o_h \ rightarrow d_3 $对称性破裂对应于经典磁性顺序,但出现在非常接近抗铁磁kitaev点的区域中,量子波动大概非常强。 In addition, a two-step symmetry breaking $O_h\rightarrow D_{3d}\rightarrow D_3$ is numerically observed as the length scale is increased: At short and intermediate length scales, the system behaves as having a rank-2 spin nematic order with $O_h\rightarrow D_{3d}$ symmetry breaking;从长距离的角度来看,时间逆转对称性进一步打破,导致$ o_h \ rightarrow d_3 $对称破坏。最后,在基塔夫阶段没有旋转顺序的数值特征,也没有Luttinger液体行为,其性质值得进一步研究。
A minimal Kitaev-Gamma model has been recently investigated to understand various Kitaev systems. In the one-dimensional Kitaev-Gamma chain, an emergent SU(2)$_1$ phase and a rank-1 spin ordered phase with $O_h\rightarrow D_4$ symmetry breaking were identified using non-Abelian bosonization and numerical techniques. However, puzzles near the antiferromagnetic Kitaev region with finite Gamma interaction remained unresolved. Here we focus on this parameter region and find that there are two new phases, namely, a rank-1 ordered phase with an $O_h\rightarrow D_3$ symmetry breaking, and a peculiar Kitaev phase. Remarkably, the $O_h\rightarrow D_3$ symmetry breaking corresponds to the classical magnetic order, but appears in a region very close to the antiferromagnetic Kitaev point where the quantum fluctuations are presumably very strong. In addition, a two-step symmetry breaking $O_h\rightarrow D_{3d}\rightarrow D_3$ is numerically observed as the length scale is increased: At short and intermediate length scales, the system behaves as having a rank-2 spin nematic order with $O_h\rightarrow D_{3d}$ symmetry breaking; and at long distances, time reversal symmetry is further broken leading to the $O_h\rightarrow D_3$ symmetry breaking. Finally, there is no numerical signature of spin orderings nor Luttinger liquid behaviors in the Kitaev phase whose nature is worth further studies.