2000
DOI: 10.1088/1009-1963/9/5/011
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The Raman scattering of carbon nanotubes produced in different inert gases and their pressures by arc discharge

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Cited by 7 publications
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“…The D* peak is unique for multiwalled carbon nanotubes. Except the strong D* band, an additional weak band is observed at 2900 cm-1 which is thought to arise from a combination of the Raman modes at 1350 cm -1 and 1580 cm -1 [21][22][23][24][25][26][27]. The spectra for SiOC also show peaks of D band and G band indicating the presence of disordered free carbon present.…”
Section: Micro-raman Spectroscopymentioning
confidence: 99%
“…The D* peak is unique for multiwalled carbon nanotubes. Except the strong D* band, an additional weak band is observed at 2900 cm-1 which is thought to arise from a combination of the Raman modes at 1350 cm -1 and 1580 cm -1 [21][22][23][24][25][26][27]. The spectra for SiOC also show peaks of D band and G band indicating the presence of disordered free carbon present.…”
Section: Micro-raman Spectroscopymentioning
confidence: 99%
“…Zhao et al [6] used H 2 -Ar atmospheres comprising 60% Ar-40% H 2 under a pressure of 266.6 mbar in their work, while Luo et al [7] and Sun et al [8] utilised high purity hydrogen at a pressure 799.9 mbar to optimize the yield in the process. Farhat et al [9], Hai-yan et al [10], and Sugai et al [11] all successfully employed an Ar atmosphere to optimize the yield of the nanotubes produced. The position of the electrode axis does not noticeably affect the MWNT quality or quantity.…”
Section: Introductionmentioning
confidence: 99%