2006
DOI: 10.1016/j.carbon.2005.10.029
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X-ray absorption near-edge structure and photoelectron spectroscopy of single-walled carbon nanotubes modified by a HBr solution

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Cited by 38 publications
(28 citation statements)
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“…In general, A and C peaks are assigned to the transition from C 1s core to CC π* and σ* states, respectively. The B peak is assigned to free‐electron‐like interlayer states in graphite or carbon nanotubes . As can be seen from the NEXAFS spectra in Figure b, the presence of a pronounced B peak indicates structural changes with the increased sp 3 ‐like structure, while the decreased intensity of A peaks demonstrates a weakening of the CC π* network.…”
Section: Resultsmentioning
confidence: 94%
“…In general, A and C peaks are assigned to the transition from C 1s core to CC π* and σ* states, respectively. The B peak is assigned to free‐electron‐like interlayer states in graphite or carbon nanotubes . As can be seen from the NEXAFS spectra in Figure b, the presence of a pronounced B peak indicates structural changes with the increased sp 3 ‐like structure, while the decreased intensity of A peaks demonstrates a weakening of the CC π* network.…”
Section: Resultsmentioning
confidence: 94%
“…X‐ray near‐edge structure (XANES) spectroscopy is an effective way to investigate the structure and composition changes. In the C 1s XANES spectrum, the distinguishable π* feature at ≈286 eV corresponding to the sp 2 bonding configuration, and feature at 293 eV is attributed to the transition of exciton from core level to σ* states . The presence of peak at 288.5 eV between π* and σ* resonances corresponds to the structure changes due to the increased sp 3 ‐like structure, with a minor contribution may come from CH at the edge or defective sites .…”
Section: Resultsmentioning
confidence: 99%
“…In the C 1s XANES spectrum, the distinguishable π* feature at ≈286 eV corresponding to the sp 2 bonding configuration, and feature at 293 eV is attributed to the transition of exciton from core level to σ* states . The presence of peak at 288.5 eV between π* and σ* resonances corresponds to the structure changes due to the increased sp 3 ‐like structure, with a minor contribution may come from CH at the edge or defective sites . With the increase of ball‐milling time, the obviously enhanced intensity of peak at 288.5 eV indicates the increased defect content, which is in well accordance with the XPS results.…”
Section: Resultsmentioning
confidence: 99%
“…In a recent report XANES was demonstrated as a very useful tool to probe the surface chemistry, degree of order, molecular orientation, and electronic structure of carbon nanotubes . Even though the origin of various XANES features was complicated, the spectral features related to different bonding states or functional groups in carbon nanomaterials have been widely discussed . Recently, XANES has been also shown to be very useful to probe the electronic structure of graphene for various applications …”
Section: Introductionmentioning
confidence: 99%