2018
DOI: 10.1016/j.carbon.2018.07.032
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Channelling and induced defects at ion-bombarded aligned multiwall carbon nanotubes

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Cited by 27 publications
(25 citation statements)
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“…Finally the component at about 286.3–287.0 eV is due to the residual C–O bond in the different possible CO configurations [ 44 , 45 , 46 ]. We underline that there is not any low-BE C 1s core-level component associated with unsaturated C dangling bonds at vacancy sites [ 10 , 23 , 68 , 69 , 70 , 71 ], not even in the deuterated sample, demonstrating the absolutely non-destructive deuteration of NPG.…”
Section: Results and Discussionmentioning
confidence: 90%
“…Finally the component at about 286.3–287.0 eV is due to the residual C–O bond in the different possible CO configurations [ 44 , 45 , 46 ]. We underline that there is not any low-BE C 1s core-level component associated with unsaturated C dangling bonds at vacancy sites [ 10 , 23 , 68 , 69 , 70 , 71 ], not even in the deuterated sample, demonstrating the absolutely non-destructive deuteration of NPG.…”
Section: Results and Discussionmentioning
confidence: 90%
“…The component at 284.2 eV is characteristic of photoelectrons emitted from carbon atoms, associated with sp 2 carbon systems in the “graphite-like” [42]. The peak reproduced at 290.5 eV is also characteristic of sp 2 carbon systems, but in this case due to the π-π* interactions and π plasmon, which is derived from the energy loss due to the excitation of π electrons [43]. Components associated with carbon in amorphous or sp 3 configuration appear at 285.0 eV [44], and defects associated with carbon vacancies appear at 282.9eV [45].…”
Section: Resultsmentioning
confidence: 99%
“…The C1s spectrum is reproduced by five components centered at binding energy 284.4 eV, 285.5 eV, 287.2 eV, 288.9 eV, and 291.4 eV (Figure 3a). The components at 284.4 eV and 291.0 eV are characteristic of sp 2 carbon systems, the first can be associated to photoelectrons emitted from carbon atoms in the carbon nanotube ‘graphite-like’ walls, while the second reflects the electron energy loss peak due to the collective excitation of π electrons, the so-called π plasmon [22,23]. The other three components are associated to photoelectrons emitted from carbon atoms at sp 3 bonds, oxygen-containing groups such as C–O and in carboxylic groups, respectively [24].…”
Section: Resultsmentioning
confidence: 99%