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Temperature dependence of the Raman spectra of multilayer graphene nanoribbons fabricated by unzipping method

机译:用解体方法制造的多层石墨烯纳米拉曼谱的温度依赖性

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The temperature dependence of Raman spectra of multilayer-graphene nanoribbons (MLGNRs) fabricated by unzipping method was investigated in the temperature range from 300 K to 700 K. MLGNRs with the width of similar to 200 nm are isolated and individually measured. The frequency of G band is monotonically downshifted with increasing temperature. The change in the G band frequency with temperature is reversible in thermal cycles with heating and cooling. By linear fitting, the temperature coefficient is estimated to be about - 0.021 cm(-1)/K. This value is smaller than - 0.028 cm(-1)/K of carbon nanotubes and larger than -0.011 and - 0.016 cm(-1)/K of graphite and graphene, respectively, as reported previously. This means that MLGNRs are thermally stable compared with carbon nanotubes with curvatures, whereas the thermal stability of MLGNRs is lower than those of graphene and graphite. The better fitting to the G band frequency shift with temperature is obtained with nonlinear quadratic curve. From the theoretical analysis of the fitted quadratic curve, it is clarified that the downshift of G band frequency with increasing temperature is attributed to the anharmonic phonon interaction, especially 4-phonon process rather than 3-phonon process. Comparing with other nanocarbon materials reported so far, it is suggested that the strength of the anharmonic phonon interaction depends on the layer number and size of graphene.
机译:在从300k至700k的温度范围内研究了通过解体方法制造的多层 - 石墨烯纳米纤维(MLGNRS)的温度依赖性,分离宽度与宽度相似的MLGNR。和单独测量。 G频段的频率随温度越来越多地下游。 G带频率的变化具有温度的热循环在加热和冷却中可逆。通过线性拟合,温度系数估计为约 - 0.021cm(-1)/ k。如前所述,该值分别小于 - 0.028cm(-1)/ k碳纳米管和大于-0.011和-011.016(-1)石墨和石墨烯。这意味着与具有曲率的碳纳米管相比,MLGNR是热稳定的,而MLGNR的热稳定性低于石墨烯和石墨的热稳定性。用非线性二次曲线获得与温度的G带频率偏移的更好的拟合。从拟合二次曲线的理论分析中,阐明了G带频率的降档,温度越来越高,归因于anharmonic声子相互作用,尤其是4-ampon过程而不是3-ampon过程。与迄今为止报道的其他纳米碳材料相比,建议anharmonic源型相互作用的强度取决于石墨烯的层数和尺寸。

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