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Using gate-modulated Raman scattering and electron-phonon interactions to probe single-layer graphene: A different approach to assign phonon combination modes

机译:使用栅极调制拉曼散射和电子 - 声子相互作用探测单层石墨烯:一种不同的方法来分配声子组合模式

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摘要

Gate-modulated and laser-dependent Raman spectroscopy have been widely used to study q = 0 zone center phonon modes, their self-energy, and their coupling to electrons in graphene systems. In this work we use gate-modulated Raman of q ≠ 0 phonons as a technique to understand the nature of five second-order Raman combination modes observed in the frequency range of 1700–2300 cm[superscript −1] of single-layer graphene (SLG). Anomalous phonon self-energy renormalization phenomena are observed in all five combination modes within this intermediate frequency region, which can clearly be distinguished from one another. By combining the anomalous phonon renormalization effect with the double resonance Raman theory, which includes both phonon dispersion relations and angular dependence of the electron-phonon scattering matrix elements, and by comparing it to the experimentally obtained phonon dispersion, measured by using different laser excitation energies, we can assign each Raman peak to the proper phonon combination mode. This approach should also shed light on the understanding of more complex structures such as few-layer graphene (FLG) and its stacking orders as well as other two-dimensional (2D)-like materials.
机译:门调制和依赖激光的拉曼光谱已被广泛用于研究q = 0区域中心声子模式,其自能以及它们与石墨烯系统中电子的耦合。在这项工作中,我们使用q≠0声子的门调制拉曼作为一种技术,以了解在单层石墨烯的1700–2300 cm [上标-1]频率范围内观察到的五个二阶拉曼组合模式的性质( SLG)。在该中频区域内,在所有五个组合模式中都观察到了异常的声子自能重整化现象。通过将异常的声子重正化效应与包含声子色散关系和电子-声子散射矩阵元素的角度依赖性的双共振拉曼理论相结合,并将其与通过使用不同的激光激发能测量的实验获得的声子色散进行比较,我们可以将每个拉曼峰分配给适当的声子组合模式。这种方法还应有助于理解更复杂的结构,例如几层石墨烯(FLG)及其堆叠顺序以及其他类似二维(2D)的材料。

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