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Laser‐induced damage and destruction of HiPCO nanotubes in different gas environments
Author(s) -
Mases Mattias,
Noël Maxime,
Dossot Manuel,
McRae Edward,
Soldatov Alexander V.
Publication year - 2011
Publication title -
physica status solidi (b)
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.51
H-Index - 109
eISSN - 1521-3951
pISSN - 0370-1972
DOI - 10.1002/pssb.201100136
Subject(s) - carbon nanotube , raman spectroscopy , materials science , argon , impurity , laser , incandescence , analytical chemistry (journal) , thermal desorption , thermal stability , nanotube , desorption , composite material , chemistry , optics , adsorption , combustion , organic chemistry , physics , soot
We have studied the thermal and chemical stability of HiPCO‐produced single‐walled carbon nanotube bundles to high laser power in air and argon. The samples were exposed to 110 kW/cm 2 during 8 h with a 1.96 eV laser and the temperature was monitored via downshift of G + ‐Raman peak. The structural changes in the carbon nanotubes (CNTs) caused by laser heating were monitored by recording their Raman spectra at ambient T (reference conditions) to ensure unaltered resonance conditions. The initial temperature was estimated to be 550 °C and 870 °C in air and argon, respectively. The Raman signal intensity from the CNTs radial breathing mode (RBM) increased rapidly at the beginning of the laser heating both under air and argon due to desorption of impurities for all but the smallest diameter CNTs. The temperature dropped by 30% under argon and 60% under air due to destruction of the absorbers – CNTs in resonance with incident radiation. The final RBM spectra exhibited intensity loss only for the smallest diameter CNTs in argon atmosphere and for all but the largest diameter CNTs in air. Our results demonstrate the importance of (i) impurity desorption from exterior and interior of CNTs; (ii) different temperature thresholds for the CNT destruction due to oxidation and overheating; (iii) the role of photon absorbers on the thermal stability of the sample. The small diameter CNTs are more easily destroyed than large diameter ones. The metallic nanotubes also tend to have lower thermal stability.

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