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arXiv 1104.2572cond-mat.str-el
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两个阿基米德晶格上的自旋半海森堡反铁磁体:从弹跳晶格到枫叶晶格及以后

The spin-half Heisenberg antiferromagnet on two Archimedian lattices: From the bounce lattice to the maple-leaf lattice and beyond

D. J. J. Farnell, R. Darradi, R. Schmidt, J. Richter

摘要:

我们研究了二维海森堡反铁磁体在两种阿基米德晶格上的基态,即枫叶晶格和弹跳晶格,以及通过改变$J'/J$从$J'/J=0$(弹跳极限)到$J'/J=1$(枫叶极限)以及更高范围内插在两种晶格之间的广义$J'$模型.我们利用耦合集团方法的高阶近似和有限格点的精确对角化,根据基态能量、磁序参量、自旋-自旋关联函数以及相邻自旋间的俯仰角等数据,讨论了基态磁长程有序.我们的研究结果表明,“纯”反弹($J'/J=0$)和枫叶($J'/J=1$)海森堡反铁磁体磁有序,然而,与子晶格磁化强度急剧减少挫折和量子涨落。我们发现,磁长程有序存在于一个广泛的参数范围$0 \le J'/J \lesssim J'_c/J $和磁序参数变化只有微弱的$J'/J$。在$J'_c \approx 1.45 J$中,发生了到量子正交二聚体单重态的直接一级跃迁,而没有磁性长程有序。正交二聚体状态是确切的基态在这个大- $J'$制度,所以我们的模型具有相似之处的Shastry-Sutherland模型。最后,我们使用精确对角化来研究磁化曲线。我们发现$J'/J \gtrsim 1.07$有一个1/3的磁化平台,而另一个在2/3饱和时的平台只出现在大的$J'/J \gtrsim 3$上。

英文摘要:

We investigate the ground state of the two-dimensional Heisenberg antiferromagnet on two Archimedean lattices, namely, the maple-leaf and bounce lattices as well as a generalized $J$-$J'$ model interpolating between both systems by varying $J'/J$ from $J'/J=0$ (bounce limit) to $J'/J=1$ (maple-leaf limit) and beyond. We use the coupled cluster method to high orders of approximation and also exact diagonalization of finite-sized lattices to discuss the ground-state magnetic long-range order based on data for the ground-state energy, the magnetic order parameter, the spin-spin correlation functions as well as the pitch angle between neighboring spins. Our results indicate that the "pure" bounce ($J'/J=0$) and maple-leaf ($J'/J=1$) Heisenberg antiferromagnets are magnetically ordered, however, with a sublattice magnetization drastically reduced by frustration and quantum fluctuations. We found that magnetic long-range order is present in a wide parameter range $0 \le J'/J \lesssim J'_c/J $ and that the magnetic order parameter varies only weakly with $J'/J$. At $J'_c \approx 1.45 J$ a direct first-order transition to a quantum orthogonal-dimer singlet ground state without magnetic long-range order takes place. The orthogonal-dimer state is the exact ground state in this large-$J'$ regime, and so our model has similarities to the Shastry-Sutherland model. Finally, we use the exact diagonalization to investigate the magnetization curve. We a find a 1/3 magnetization plateau for $J'/J \gtrsim 1.07$ and another one at 2/3 of saturation emerging only at large $J'/J \gtrsim 3$.

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