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Resonant scattering by magnetic impurities as a model for spin relaxation in bilayer graphene

机译:磁性杂质的共振散射作为旋转模型   双层石墨烯中的松弛

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摘要

We propose that the observed spin-relaxation in bilayer graphene is due toresonant scattering by magnetic impurities. We analyze a resonant scatteringmodel due to adatoms on both dimer and non-dimer sites, finding that only theformer give narrow resonances at the charge neutrality point. Opposite tosingle-layer graphene, the measured spin-relaxation rate in graphene bilayerincreases with carrier density. Although it has been commonly argued that adifferent mechanism must be at play for the two structures, our model explainsthis behavior rather naturally in terms of different broadening scales for thesame underlying resonant processes. Not only our results---using robust andfirst-principles inspired parameters---agree with experiment, they also predictan experimentally testable sharp decrease of the spin-relaxation rate at highcarrier densities.
机译:我们提出,在双层石墨烯中观察到的自旋弛豫是由于磁性杂质引起的共振散射。我们分析了由于二聚体和非二聚体位点上的原子均存在的原子引起的共振散射模型,发现只有前者在电荷中性点处给出窄的共振。与单层石墨烯相反,石墨烯双层中测得的自旋弛豫速率随载流子密度的增加而增加。尽管通常认为这两种结构必须发挥不同的作用机理,但我们的模型以相同的基础共振过程的不同扩展尺度自然地解释了这种行为。不仅我们的结果-使用可靠且第一原则启发的参数-均与实验相符,而且还预测了在高载流子密度下自旋松弛速率的实验可测试的急剧下降。

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