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Inducing Kondo screening of vacancy magnetic moments in graphene with gating and local curvature

机译:通过门控和局部曲率诱导Kondo筛选石墨烯中的空位磁矩

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摘要

In normal metals the magnetic moment of impurity-spins disappears below a characteristic Kondo temperature which marks the formation of a cloud of conduction-band electrons that screen the local-moment. In contrast, moments embedded in insulators remain unscreened at all temperatures. What then is the fate of magnetic-moments in intermediate, pseudogap systems, such as graphene? Theory predicts that coupling to the conduction-band electrons will drive a quantum phase transition between a local-moment phase and a Kondo-screened phase. However, attempts to experimentally confirm this prediction and its intriguing consequences, such as electrostatically tunable magnetic-moments, have been elusive. Here we report the observation of Kondo-screening and the quantum phase-transition between screened and unscreened phases of vacancy magnetic moments in graphene. Using scanning tunneling spectroscopy and numerical renormalization-group calculations we show that this transition enables to control the screening of local moments by tuning the gate voltage and the local curvature of the graphene membrane.
机译:在普通金属中,自旋的磁矩在特征性的近藤温度以下消失,这标志着形成屏蔽局部矩的导带电子云的形成。相反,绝缘子中嵌入的力矩在所有温度下均不受屏蔽。那么在中间的伪间隙系统(例如石墨烯)中,磁矩的命运是什么?理论预测,与导带电子的耦合将驱动量子矩在局部矩相与近藤屏蔽相之间的跃迁。然而,尝试通过实验确认该预测及其令人感兴趣的结果,例如静电可调磁矩,一直难以捉摸。在这里,我们报告观察到的近藤屏蔽和石墨烯中空磁矩的已屏蔽和未屏蔽相之间的量子相变。使用扫描隧道光谱和数值归一化组计算,我们表明,这种转变能够通过调节栅极电压和石墨烯膜的局部曲率来控制局部矩的屏蔽。

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