Univ. Lyon, Université Claude Bernard Lyon 1, CNRS, Institut Lumire Matière , F-69622, Villeurbanne, France.
Departamento de Física, Campus Ministro Petrônio Portella, Universidade Federal do Piauí , Teresina, Piauí 64049-550, Brazil.
Nano Lett. 2017 Jan 11;17(1):21-27. doi: 10.1021/acs.nanolett.6b02981. Epub 2016 Dec 7.
Understanding the mechanism and limits of strain transfer between supported 2D systems and their substrate is a most needed step toward the development of strain engineering at the nanoscale. This includes applications in straintronics, nanoelectromechanical devices, or new nanocomposites. Here, we have studied the limits of biaxial compressive strain transfer among SiO, diamond, and sapphire substrates and graphene. Using high pressure-which allows maximizing the adhesion between graphene and the substrate on which it is deposited-we show that the relevant parameter governing the graphene mechanical response is not the applied pressure but rather the strain that is transmitted from the substrate. Under these experimental conditions, we also show the existence of a critical biaxial stress beyond which strain transfer become partial and introduce a parameter, α, to characterize strain transfer efficiency. The critical stress and α appear to be dependent on the nature of the substrate. Under ideal biaxial strain transfer conditions, the phonon Raman G-band dependence with strain appears to be linear with a slope of -60 ± 3 cm/% down to biaxial strains of -0.9%. This evolution appears to be general for both biaxial compression and tension for different experimental setups, at least in the biaxial strain range -0.9% < ε < 1.8%, thus providing a criterion to validate total biaxial strain transfer hypotheses. These results invite us to cast a new look at mechanical strain experiments on deposited graphene as well as to other 2D layered materials.
理解支撑二维(2D)系统与其衬底之间应变传递的机制和限制,是向纳米尺度应变工程发展迈出的最必要的一步。这包括在应变电子学、纳米机电设备或新型纳米复合材料中的应用。在这里,我们研究了 SiO2、金刚石和蓝宝石衬底与石墨烯之间双轴压缩应变传递的极限。利用高压——这允许最大限度地提高石墨烯与沉积其上的衬底之间的附着力——我们表明,控制石墨烯力学响应的相关参数不是所施加的压力,而是从衬底传递的应变。在这些实验条件下,我们还证明了存在一个超过该值的双轴临界应力,超过该值应变传递会变得部分,并且引入一个参数α来表征应变传递效率。临界应力和α似乎取决于衬底的性质。在理想的双轴应变传递条件下,应变的声子 Raman G 带依赖性似乎呈线性关系,斜率为-60±3cm/%,直到双轴应变-0.9%。这种演变似乎对于不同的实验设置,无论是双轴压缩还是拉伸,都是普遍的,至少在双轴应变范围-0.9%<ε<1.8%,从而为验证总双轴应变传递假设提供了一个标准。这些结果促使我们重新审视沉积石墨烯以及其他二维层状材料的机械应变实验。