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Magnetic nanopantograph in the SrCu2(BO3)2 Shastry–Sutherland lattice

机译:SrCu2(BO3)2 Shastry-Sutherland晶格中的磁性纳米受电弓

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摘要

Magnetic materials having competing, i.e., frustrated, interactions can display magnetism prolific in intricate structures, discrete jumps, plateaus, and exotic spin states with increasing applied magnetic fields. When the associated elastic energy cost is not too expensive, this high potential can be enhanced by the existence of an omnipresent magnetoelastic coupling. Here we report experimental and theoretical evidence of a nonnegligible magnetoelastic coupling in one of these fascinating materials, SrCu2(BO3)2 (SCBO). First, using pulsed-field transversal and longitudinal magnetostriction measurements we show that its physical dimensions, indeed, mimic closely its unusually rich field-induced magnetism. Second, using density functional-based calculations we find that the driving force behind the magnetoelastic coupling is the CuOCu^ superexchange angle that, due to the orthogonal Cu2+ dimers acting as pantographs, can shrink significantly (0.44%) with minute (0.01%) variations in the lattice parameters. With this original approach we also find a reduction of ∼10% in the intradimer exchange integral J, enough to make predictions for the highly magnetized states and the effects of applied pressure on SCBO.
机译:具有竞争性(即受挫的)相互作用的磁性材料可以在复杂的结构,离散的跃迁,平稳和奇特的自旋态下,随着施加的磁场的增加而表现出丰富的磁性。当相关的弹性能量成本不太昂贵时,可以通过存在无所不在的磁弹性耦合来增强这种高潜力。在这里,我们报告在这些迷人的材料之一SrCu2(BO3)2(SCBO)中不可忽略的磁弹性耦合的实验和理论证据。首先,我们使用脉冲场横向和纵向磁致伸缩测量结果表明,其物理尺寸确实紧密模拟了其异常丰富的磁场感应磁场。其次,使用基于密度泛函的计算,我们发现磁弹性耦合背后的驱动力是 CuOCu ^ 的超交换角,由于正交的Cu 2 + 二聚体充当受电弓,因此可以显着收缩(0.44%),且变化很小(0.01%)。晶格参数。通过这种原始方法,我们还发现二聚体内部交换积分J降低了约10%,足以预测高磁化状态以及施加压力对SCBO的影响。

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