Institute of Physics, Chinese Academy of Sciences , Beijing 100190, China.
Nano Lett. 2014 Jul 9;14(7):4011-5. doi: 10.1021/nl501425n. Epub 2014 Jun 11.
The Kondo effect, a widely studied phenomenon in which the scattering of conduction electrons by magnetic impurities increases as the temperature T is lowered, depends strongly on the density of states at the Fermi energy. It has been predicted by theory that magnetic impurities on free-standing monolayer graphene exhibit the Kondo effect and that control of the density of states at the Fermi level by external means can be used to switch the effect on and off. However, though transport data for Co adatoms on graphene monolayers on several substrates have been reported, there exists no evidence for a Kondo effect. Here we probe the role of the substrate on the Kondo effect of Co on graphene by combining low-temperature scanning tunneling microscopy and spectroscopy measurements with density functional theory calculations. We use a Ru(0001) substrate that is known to cause graphene to ripple, yielding a moiré superlattice. The experimental data show a sharp Kondo resonance peak near the Fermi energy from only Co adatoms at the edge of atop regions of the moiré pattern. The theoretical results show that the variation of the distance from the graphene to the Ru substrate, which controls the spin polarization and local density of states at the Fermi energy, is the key factor for the appearance of the Kondo resonance. The results suggest that rippling of graphene by suitable substrates is an additional lever for tuning and selectively switching the appearance of the Kondo effect.
近藤效应是一种广泛研究的现象,即在温度 T 降低时,传导电子被磁性杂质散射的程度增加,它强烈依赖于费米能级处的态密度。理论预测,自由-standing 单层石墨烯上的磁性杂质表现出近藤效应,并且通过外部手段控制费米能级处的态密度可以用来打开和关闭该效应。然而,尽管已经报道了几种衬底上石墨烯单层上 Co 原子吸附体的输运数据,但没有近藤效应的证据。在这里,我们通过低温扫描隧道显微镜和光谱测量与密度泛函理论计算相结合,研究了衬底对 Co 在石墨烯上的近藤效应的影响。我们使用了已知会导致石墨烯产生波纹,从而产生莫尔超晶格的 Ru(0001)衬底。实验数据显示,在莫尔图案的 atop 区域边缘的 Co 原子吸附体上,仅在费米能级附近出现了尖锐的近藤共振峰。理论结果表明,控制费米能级处自旋极化和局域态密度的石墨烯与 Ru 衬底之间的距离的变化是出现近藤共振的关键因素。这些结果表明,通过合适的衬底使石墨烯产生波纹是调节和选择性切换近藤效应出现的另一个手段。