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Excitonic Magnetism in Van Vleck-type d~4 Mott Insulators

机译:Van Vleck型d〜4 Mott绝缘子的激磁磁性

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摘要

In Mott insulators with the t~4_(2g) electronic configuration such as of Re~(3+), Ru~(4+), Os~(4+), and Ir~(5+) ions, spin-orbit coupling dictates a Van Vleck-type nonmagnetic ground state with an angular momentum J = 0, and the magnetic response is governed by gapped singlet-triplet excitations. We derive the exchange interactions between these excitons and study their collective behavior on different lattices. In perovskites, a conventional Bose condensation of excitons into a magnetic state is found, while an unexpected one-dimensional behavior supporting spin-liquid states emerges in honeycomb lattices, due to the bond directional nature of exciton interactions in the case of 90° d-p-d bonding geometry.
机译:在具有t〜4_(2g)电子结构的Mott绝缘子中,例如Re〜(3 +),Ru〜(4 +),Os〜(4+)和Ir〜(5+)离子,自旋轨道耦合决定了角动量为J = 0的Van Vleck型非磁性基态,磁响应由有间隙的单重态-三重态激发控制,我们得出了这些激子之间的交换相互作用,并研究了它们在不同晶格上的集体行为。发现了激子的常规玻色缩合成磁性态,而在90°dpd键合几何形状的情况下,由于激子相互作用的键方向性质,在蜂窝晶格中出现了支持自旋液体态的意外的一维行为。

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