Stokes/anti‐Stokes Raman Spectroscopy of HiPco Single‐Wall Carbon Nanotubes

E. Gregan, S. Keogh, T. Hedderman, B. McCarthy, Garrett F. Farrell, G. Chambers, H. Byrne
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引用次数: 5

Abstract

An analysis of the Raman spectra of single‐walled HiPco carbon nanotube powder using laser energies of 1.92 eV, 2.4 eV, 2.5 eV and 2.7 eV, including a comparison of the Stokes and anti‐Stokes contributions is presented. The diameter distribution was determined to be 0.8 – 1.2 nm from the spectral positioning of the Radial Breathing Modes. The diameter distribution is consistent with that determined by NIR absorption spectroscopy. At all excitation energies the profile of the G‐line (≈ 1580cm−1) indicates a predominance of semiconducting tubes although at 2.4 eV there is some indication of some contribution from metallic tubes. In all cases the anti Stokes line was weak and the Stokes/anti Stokes ratio was at least an order of magnitude indicating at most weak resonance enhancement in either.
HiPco单壁碳纳米管的Stokes/anti - Stokes拉曼光谱
利用1.92 eV、2.4 eV、2.5 eV和2.7 eV的激光能量对单壁HiPco碳纳米管粉末的拉曼光谱进行了分析,并对Stokes贡献和反Stokes贡献进行了比较。根据径向呼吸模式的光谱定位确定直径分布在0.8 - 1.2 nm之间。直径分布与近红外吸收光谱测定结果一致。在所有激发能下,G线轮廓(≈1580cm−1)表明半导体管占主导地位,尽管在2.4 eV处有一些来自金属管的贡献。在所有情况下,反Stokes线都是弱的,Stokes/反Stokes比至少是一个数量级,这表明在任何一种情况下都有最弱的共振增强。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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