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Spin-orbit coupling in octamers in a spinel sulfide CuIr$_2$S$_4$: Competition between spin-singlet and quadrupolar states, and its relevance to remnant paramagnetism

机译:尖晶石硫化物中八聚体中的自旋轨道耦合CuIr $ _2 $ s $ _4 $:   自旋单线态和四极态之间的竞争及其与...的相关性   残余的顺磁性

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摘要

We theoretically investigate magnetic properties in the low-temperature phasewith the formation of eight-site clusters, octamers, in the spinel compoundCuIr$_2$S$_4$. The octamer state was considered to be a spin-singlet stateinduced by a Peieirls instability through the strong anisotropy of $d$orbitals, the so-called orbital Peierls state. We reexamine this picture bytaking into account the spin-orbit coupling which was ignored in the previousstudy. We derive a low-energy effective model between $j_{\rm eff}=1/2$quasispins on Ir$^{4+}$ cations in an octamer from the multiorbital Hubbardmodel with the strong spin-orbit coupling by performing the perturbationexpansion from the strong correlation limit. The effective Hamiltonian is inthe form of the Kitaev-Heisenberg model but with an additional interaction, asymmetric off-diagonal exchange interaction originating from the perturbationprocess including both d-d and d-p-d hopping. Analyzing the effectiveHamiltonian on two sites and the octamer by the exact diagonalization, we findthat there is a competition between a spin-singlet state and a quadrupolarstate. The former singlet state is a conventional one, adiabatically connectedto the orbital-Peierls state. On the other hand, the latter quadrupolar stateis stabilized by the additional interaction, which consists of a linearcombination of different total spin momenta along the spin quantization axis.In the competing region, the model exhibits paramagnetic behavior with arenormalized small effective moment at low temperature. This peculiar remnantparamagnetism is not obtained in the Kitaev-Heisenberg model without theadditional interaction. Our results renew the picture of the octamer state andprovide a scenario for the intrinsic paramagnetic behavior recently observed ina muon spin rotation experiment [K. M. Kojima et al., Phys. Rev. Lett. 112,087203 (2014)].
机译:我们从理论上研究了在尖晶石化合物CuIr $ _2 $ S $ _4 $中形成八点簇八聚体的低温阶段的磁性。八面体状态被认为是由Peieirls不稳定性通过$ d $轨道的强各向异性(所谓的轨道Peierls状态)引起的自旋单态。我们通过考虑在先前研究中被忽略的自旋-轨道耦合来重新检查这张图。我们通过执行扰动展开,从八轨道多巴哈伯德模型中获得强自旋轨道耦合的八聚体中Ir $ ^ {4 +} $阳离子上的$ j _ {\ rm eff} = 1/2 $ quasispins之间的低能效模型从强相关极限。有效的哈密顿量为Kitaev-Heisenberg模型的形式,但具有附加的相互作用,即源自d-d和d-p-d跳跃的扰动过程的非对称非对角交换相互作用。通过精确的对角化分析两个位置上的有效哈密顿量和八面体,我们发现自旋-单重态与四极态之间存在竞争。前者的单重态是常规的,绝热地连接到轨道-皮埃尔斯态。另一方面,后者的四极态通过额外的相互作用而得以稳定,该相互作用由沿着自旋量化轴的不同总自旋矩的线性组合组成。在竞争区域中,模型表现出顺磁行为,且在低温下具有标准化的小有效矩。没有额外的相互作用,在Kitaev-Heisenberg模型中无法获得这种特殊的剩余顺磁性。我们的结果更新了八聚体态的图景,并为最近在介子自旋旋转实验中观察到的固有顺磁行为提供了一种方案[K.小岛M.牧师112,087203(2014)]。

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    Nasu, Joji; Motome, Yukitoshi;

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