Hussein Siham M, Crowe Iain F, Clark Nick, Milosevic Milan, Vijayaraghavan Aravind, Gardes Frederic Y, Mashanovich Goran Z, Halsall Matthew P
Photon Science Institute and School of Electrical and Electronic Engineering, University of Manchester, Manchester, M13 9PL, UK.
School of Materials and the National Graphene Institute, University of Manchester, Manchester, M13 9PL, UK.
Nanoscale Res Lett. 2017 Nov 22;12(1):600. doi: 10.1186/s11671-017-2374-4.
We present a Raman mapping study of monolayer graphene G and 2D bands, after integration on silicon strip-waveguide-based micro-ring resonators (MRRs) to characterize the effects of the graphene transfer processes on its structural and optoelectronic properties. Analysis of the Raman G and 2D peak positions and relative intensities reveal that the graphene is electrically intrinsic where it is suspended over the MRR but is moderately hole-doped where it sits on top of the waveguide structure. This is suggestive of Fermi level 'pinning' at the graphene-silicon heterogeneous interface, and we estimate that the Fermi level shifts down by approximately 0.2 eV from its intrinsic value, with a corresponding peak hole concentration of ~ 3 × 10 cm. We attribute variations in observed G peak asymmetry to a combination of a 'stiffening' of the E optical phonon where the graphene is supported by the underlying MRR waveguide structure, as a result of this increased hole concentration, and a lowering of the degeneracy of the same mode as a result of localized out-of-plane 'wrinkling' (curvature effect), where the graphene is suspended. Examination of graphene integrated with two different MRR devices, one with radii of curvature r = 10 μm and the other with r = 20 μm, indicates that the device geometry has no measureable effect on the level of doping.
我们展示了一项关于单层石墨烯G和2D带的拉曼映射研究,该研究是在基于硅条形波导的微环谐振器(MRR)上集成之后进行的,目的是表征石墨烯转移过程对其结构和光电特性的影响。对拉曼G峰和2D峰的位置以及相对强度的分析表明,石墨烯在悬浮于MRR上方时是本征态的,但在位于波导结构顶部时是适度空穴掺杂的。这表明费米能级在石墨烯 - 硅异质界面处被“钉扎”,我们估计费米能级从其本征值向下移动约0.2 eV,相应的峰值空穴浓度约为3×10¹² cm⁻³。我们将观察到的G峰不对称性变化归因于以下因素的组合:由于空穴浓度增加,在石墨烯由底层MRR波导结构支撑的地方,E光学声子发生“硬化”;以及在石墨烯悬浮的地方,由于局部面外“起皱”(曲率效应)导致同一模式的简并度降低。对与两种不同MRR器件集成的石墨烯进行检查,一种器件的曲率半径r = 10μm,另一种器件的r = 20μm,结果表明器件几何形状对掺杂水平没有可测量的影响。