Untitled - IAP/TU Wien - Technische Universität Wien
Untitled - IAP/TU Wien - Technische Universität Wien
Untitled - IAP/TU Wien - Technische Universität Wien
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Nanostructure Characterisation by Electron Beam Techniques<br />
Multi-walled carbon nanotubes irradiated by proton beams:<br />
An energy loss study<br />
Isabel Abril 1,* , Jorge E. Valdés 2 , Rafael Garcia-Molina 3 , Carlos Celedón 2,4 , Rodrigo Segura 5 , Néstor<br />
R. Arista 4 , Patricio Vargas 2<br />
1 Departament de Física Aplicada, Universitat d’Alacant, E-03080 Alacant, Spain<br />
2 Departamento de Física – Laboratorio de Colisiones Atómicas, Universidad Técnica Federico Santa María<br />
(UTFSM), Valparaíso 2390123, Chile<br />
3 Departamento de Física – Centro de Investigación en Óptica y Nanofísica, Universidad de Murcia, E-30100<br />
Murcia, Spain<br />
4 Centro Atómico Bariloche, División Colisiones Atómicas, RA-8400 S. C. de Bariloche, Argentina<br />
5 Departamento de Química y Bioquímica, Facultad de Ciencias, Universidad de Valparaíso, Chile<br />
*corresponding author ias@ua.es (Isabel Abril)<br />
The irradiation with energetic proton beams impinging normal to the axis of a multiwalled carbon nanotube<br />
(MWCNT) is studied both experimental and theoretically, in the keV energy range. The MWCNTs are<br />
dispersed on top of a very thin film of holey amorphous carbon (a-C) substrate. Measurements of the proton<br />
energy loss distribution at the forward direction are performed by the transmission technique, obtaining energy<br />
loss spectra with two well differentiated peaks.<br />
A semi-classical simulation is employ to elucidate the origin of the peaks in the energy distribution. The<br />
simulation follows the trajectories of each projectile by solving its equation of motion, where the electronic<br />
stopping force was accounted for by a non-linear density functional formalism depending on the local<br />
electronic density.<br />
By the simulation we predict that the experimental low-energy-loss peak is due to protons moving in<br />
quasi-channelling between the most external walls of the MWCNTs. The experimental high-energy-loss peak<br />
are those channelled protons, with larger impact parameter and small angular dispersion after traversing the<br />
a-C film, which can reach the detector at zero angle with only an extra energy loss that shifts to a lower<br />
energy their energy distribution [1].<br />
[1] J. E. Valdés, C. Celedón, R. Segura, I. Abril, R. Garcia-Molina, C. D. Denton, N. R. Arista and P. Vargas,<br />
Carbon 52 (2013)137.<br />
Acknowledgments: This work has been financially supported by the following Grants: Fondecyt 1100759<br />
and USM-DGIP 11.11.11, Financiamiento Basal para Centros Científicos y Tecnológicos de Excelencia<br />
(CEDENNA), the Spanish Ministerio de Economía y Competitividad and the European Regional<br />
Development Fund (Project FIS2010-17225).<br />
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