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Edge state magnetism in zigzag-interfaced graphene via spin susceptibility measurements

机译:通过自旋磁化率测量曲折界面石墨烯的边缘态磁性

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摘要

Development of graphene spintronic devices relies on transforming it into a material with a spin order. Attempts to make graphene magnetic by introducing zigzag edge states have failed due to energetically unstable structure of torn zigzag edges. Here, we report on the formation of nanoridges, i.e., stable crystallographically oriented fluorine monoatomic chains, and provide experimental evidence for strongly coupled magnetic states at the graphene-fluorographene interfaces. From the first principle calculations, the spins at the localized edge states are ferromagnetically ordered within each of the zigzag interface whereas the spin interaction across a nanoridge is antiferromagnetic. Magnetic susceptibility data agree with this physical picture and exhibit behaviour typical of quantum spin-ladder system with ferromagnetic legs and antiferromagnetic rungs. The exchange coupling constant along the rungs is measured to be 450 K. The coupling is strong enough to consider graphene with fluorine nanoridges as a candidate for a room temperature spintronics material.
机译:石墨烯自旋电子器件的开发依赖于将其转化为具有自旋顺序的材料。通过引入锯齿形边缘状态来使石墨烯磁性的尝试由于撕裂的锯齿形边缘的能量不稳定结构而失败。在这里,我们报告了纳米脊的形成,即稳定的晶体学取向的氟单原子链,并为石墨烯-氟代石墨烯界面上强耦合的磁态提供了实验证据。从第一原理计算中,在每个锯齿形界面内,局部边缘状态的自旋是铁磁有序的,而跨纳米脊的自旋相互作用是反铁磁的。磁化率数据与此物理图像相符,并显示出具有铁磁腿和反铁磁梯级的量子自旋梯系统的典型行为。沿横档的交换耦合常数测得为450 K,耦合强度足以考虑将具有氟纳米脊的石墨烯用作室温自旋电子材料的候选材料。

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