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Frustration in Ising-type spin models on the pyrochlore lattice

机译:烧绿石晶格上伊辛型自旋模型的失意

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We compare the behaviour of ferromagnetic and antiferromagnetic Ising-type spin models on the cubic pyrochlore lattice. With simple 'up-down' Ising spins, the antiferromagnet is highly frustrated and the ferromagnet is not. However, such spin symmetry cannot be realized on the pyrochlore lattice, since it requires a unique symmetry axis, which is incompatible with the cubic symmetry. The only two-state spin symmetry which is compatible is that with four local (1 1 1) anisotropy axes, which direct the spins to point in or out of the tetrahedral plaquettes of the pyrochlore lattice. We: show how the local 'in-out' magnetic anisotropy reverses the roles of the ferro-and antiferromagnetic exchange couplings with regard to frustration, such that the ferromagnet is highly frustrated and the antiferromagnet is not. The in-out ferromagnet is a magnetic analogue of the ice model, which we have termed the 'spin ice model'. it is realized in the material Ho2Ti2O7. The up-down antiferromagnet is also an analogue of the ice model, albeit a less direct one, as originally shown by Anderson. Combining these results shows that the up-down spin models map onto the in-out spin models with the opposite sign of the exchange coupling. We present Mont : Carlo simulations of the susceptibility for each model, and discuss their relevance to experimental systems. [References: 17]
机译:我们在立方烧绿石晶格上比较了铁磁和反铁磁Ising型自旋模型的行为。通过简单的“上下” Ising自旋,反铁磁体非常受挫,而铁磁体却没有。但是,这种自旋对称性不能在烧绿石晶格上实现,因为它需要唯一的对称轴,而该轴与立方对称性不兼容。唯一可兼容的两种状态的自旋对称性是具有四个局部(1 1 1)各向异性轴的,该轴将自旋指向指向或指向烧绿石晶格的四面体薄片。我们:展示了局部“由内而外”的磁各向异性如何逆转了铁磁和反铁磁交换耦合在挫折方面的作用,从而使铁磁极受挫而反铁磁却没有。进出铁磁体是冰模型的磁性类似物,我们称其为“自旋冰模型”。它由材料Ho2Ti2O7实现。上下反铁磁体也是冰模型的类似物,尽管不那么直接,就像安德森最初展示的那样。组合这些结果表明,上下自旋模型映射到具有交换耦合相反符号的内向自旋模型。我们介绍每个模型的磁化率的Mont:Carlo模拟,并讨论它们与实验系统的相关性。 [参考:17]

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