首页> 外文会议>International Conference on Science and Application of Nanotubes Jul 24-27, 1999, East Lansing, Michigan >FIRST AND SECOND-ORDER RESONANT RAMAN SPECTRA OF SINGLE-WALLED CARBON NANOTUBES
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FIRST AND SECOND-ORDER RESONANT RAMAN SPECTRA OF SINGLE-WALLED CARBON NANOTUBES

机译:单壁碳纳米管的一阶和二阶共振拉曼光谱

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In summary, overtones and combination modes have been identified in the second-order spectra for the two dominant features in the first-order spectra (the radial breathing mode and the tangential mode) that are associated with the resonant Raman enhance-ment process arising from the 1D electronic density of states. Just as for the case of the first-order spectra, the resonant contributions to the second-order spectra also involve a different set of (n, m) nanotubes at each laser excitation energy E_(laser). A second-order analog is observed for the broad spectral band identified with contributions from metallic nanotubes to the first-order tangential mode spectra. The unique feature of the second-order tangential overtone band shows a larger E_(laser) range over which the metallic nanotubes contribute, and this effect is attributed to the large (hω_(phonon) ~ 0.4eV) energy of these phonons. Combination modes associated with (ω_(tang) + ωRBM) and (ωtang + 2ωRBM) have been identified. These combination modes show behaviors as a function of E_(laser) that are consistent with the behavior of their first-order constituents, namely that different nanotubes contribute to the spectra at each value of E_(laser). The behavior of the 'D-band' and G'-band features show a very large phonon frequency dependence on E_(laser), and show a resonant 2D behavior when the electron and phonon wave vectors coincide, as also occurs in other sp~2 carbons. Future Raman studies are likely to explore the relation between the Stokes and the anti-Stokes spectra as a function of E_(laser). Surface-enhanced Raman scattering (SERS) is likely to be explored as a method for achieving much higher sensitivity, allowing exploration of the vibrational spectra of a small number of nanotubes and perhaps even eventually the Raman spectrum of a single nanotube.
机译:总之,在二阶频谱中已针对与共振拉曼增强过程相关的一阶频谱中的两个主要特征(径向呼吸模式和切向模式)识别了泛音和组合模式。一维电子状态密度。就像一阶光谱的情况一样,对二阶光谱的共振贡献在每个激光激发能E_(laser)处也涉及一组不同的(n,m)纳米管。对于由金属纳米管对一阶切向模式光谱的贡献所识别的宽光谱带,观察到了二阶类似物。二阶切向泛音带的独特特征显示出较大的E_(激光)范围,金属纳米管在该范围内起作用,并且这种效应归因于这些声子的大(hω_(声子)〜0.4eV)能量。已经确定了与(ω_(tang)+ωRBM)和(ωtang+2ωRBM)相关的组合模式。这些组合模式显示的行为是E_(激光)的函数,与它们的一阶成分的行为一致,即不同的纳米管对E_(激光)的每个值的光谱都有贡献。 “ D波段”和“ G波段”特征的行为表现出非常大的声子频率对E_(激光)的依赖性,并且在电子和声子波矢量重合时表现出共振的二维行为,这在其他sp〜 2个碳。未来的拉曼研究可能会探索斯托克斯光谱和反斯托克斯光谱之间的关系,并将其作为E_(激光)的函数。表面增强拉曼散射(SERS)可能会被视为获得更高灵敏度的方法,从而允许探索少量纳米管的振动光谱,甚至可能最终探究单个纳米管的拉曼光谱。

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