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Evidence for Spin Glass Ordering Near the Weak to Strong Localization Transition in Hydrogenated Graphene

机译:氢化石墨烯中从弱到强的局部转变附近的自旋玻璃有序的证据

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We provide evidence that magnetic moments formed when hydrogen atoms are covalently bound to graphene exhibit spin glass ordering. We observe logarithmic time-dependent relaxations in the remnant magnetoresistance following magnetic field sweeps, as well as strong variances in the remnant magnetoresistance following field-cooled and zero-field-cooled scenarios, which are hallmarks of canonical spin glasses and provide experimental evidence for the hydrogenated graphene spin glass state. Following magnetic field sweeps, and over a relaxation period of several minutes, we measure changes in the resistivity that are more than 3 orders of magnitude larger than what has previously been reported for a two-dimensional spin glass. Magnetotransport measurements at the Dirac point, and as a function of hydrogen concentration, demonstrate that the spin glass state is observable as the zero-field resistivity reaches a value close to the quantum unit h/2e(2), corresponding to the point at which the system undergoes a transition from weak to strong localization. Our work sheds light on the critical magnetic-dopant density required to observe spin glass formation in two-dimensional systems. These findings have implications to the basic understanding of spin glasses as well the fields of two-dimensional magnetic materials and spintronics.
机译:我们提供的证据表明,当氢原子与石墨烯共价结合时形成的磁矩表现出自旋玻璃有序化。我们观察到磁场扫描后残余磁阻的对数时间依赖性弛豫,以及场冷却和零场冷却后残余磁阻的强方差,这是规范自旋玻璃的标志,并为标准自旋玻璃提供了实验证据。氢化石墨烯自旋玻璃态。在磁场扫描之后,经过几分钟的弛豫时间,我们测得的电阻率变化比二维旋转玻璃的电阻率变化大3个数量级。在狄拉克点的磁传输测量以及氢浓度的函数表明,随着零场电阻率达到接近量子单位h / 2e(2)的值(对应于该点),自旋玻璃态是可观察到的。系统经历了从弱本地化到强本地化的转变。我们的工作阐明了观察二维系统中旋转玻璃形成所需的临界磁掺杂密度。这些发现对自旋玻璃以及二维磁性材料和自旋电子学领域的基本理解具有影响。

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