School of Physics and Astronomy, University of Leeds, Leeds LS2 9JT, UK.
Stephenson Institute for Renewable Energy, Department of Chemistry, University of Liverpool, Liverpool L69 3BX, UK.
Nature. 2015 Aug 6;524(7563):69-73. doi: 10.1038/nature14621.
Only three elements are ferromagnetic at room temperature: the transition metals iron, cobalt and nickel. The Stoner criterion explains why iron is ferromagnetic but manganese, for example, is not, even though both elements have an unfilled 3d shell and are adjacent in the periodic table: according to this criterion, the product of the density of states and the exchange integral must be greater than unity for spontaneous spin ordering to emerge. Here we demonstrate that it is possible to alter the electronic states of non-ferromagnetic materials, such as diamagnetic copper and paramagnetic manganese, to overcome the Stoner criterion and make them ferromagnetic at room temperature. This effect is achieved via interfaces between metallic thin films and C60 molecular layers. The emergent ferromagnetic state exists over several layers of the metal before being quenched at large sample thicknesses by the material's bulk properties. Although the induced magnetization is easily measurable by magnetometry, low-energy muon spin spectroscopy provides insight into its distribution by studying the depolarization process of low-energy muons implanted in the sample. This technique indicates localized spin-ordered states at, and close to, the metal-molecule interface. Density functional theory simulations suggest a mechanism based on magnetic hardening of the metal atoms, owing to electron transfer. This mechanism might allow for the exploitation of molecular coupling to design magnetic metamaterials using abundant, non-toxic components such as organic semiconductors. Charge transfer at molecular interfaces may thus be used to control spin polarization or magnetization, with consequences for the design of devices for electronic, power or computing applications (see, for example, refs 6 and 7).
过渡金属铁、钴和镍。斯通纳准则解释了为什么铁是铁磁性的,而锰则不是,尽管这两种元素都有一个未填满的 3d 壳层,并且在元素周期表中相邻:根据这一准则,态密度和交换积分的乘积必须大于 1,才能出现自发自旋有序。在这里,我们证明了改变非铁磁材料(如抗磁性的铜和顺磁性的锰)的电子态是可能的,可以克服斯通纳准则,使它们在室温下具有铁磁性。这种效应是通过金属薄膜和 C60 分子层之间的界面实现的。在大块材料的体性质使样品厚度较大时,金属的几个层中存在的铁磁态被猝灭之前,该铁磁态存在。虽然磁强计可以很容易地测量感应磁化,但低能μ子自旋光谱通过研究植入样品中的低能μ子的去极化过程,可以提供其分布的深入了解。该技术表明,在金属-分子界面处和附近存在局域自旋有序态。密度泛函理论模拟表明,由于电子转移,金属原子的磁硬化是一种基于磁性硬化的机制。这种机制可能允许利用分子耦合来设计使用丰富、无毒的组件(如有机半导体)的磁性超材料。因此,分子界面处的电荷转移可以用于控制自旋极化或磁化,这对电子、电力或计算应用的器件设计有影响(例如,参见参考文献 6 和 7)。