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2006
DOI: 10.1016/j.susc.2005.12.070
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Size and temperature dependence of the specific heat capacity of carbon nanotubes

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Cited by 76 publications
(44 citation statements)
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“…As the temperature rises the 1 st optical subband g SW (30 K) is being occupied and the character of the dependence C(T) changes from one -dimensional to quasi -two -dimensional. According to theory [1,2], in this case the crossover temperature T c increases as the SWNT diameter decreases. T c can be estimated as T c  E 1 sub /6k B , where k B is the Boltzmann constant [8,11].…”
Section: Resultsmentioning
confidence: 97%
“…As the temperature rises the 1 st optical subband g SW (30 K) is being occupied and the character of the dependence C(T) changes from one -dimensional to quasi -two -dimensional. According to theory [1,2], in this case the crossover temperature T c increases as the SWNT diameter decreases. T c can be estimated as T c  E 1 sub /6k B , where k B is the Boltzmann constant [8,11].…”
Section: Resultsmentioning
confidence: 97%
“…This model is more realistic than previous random walk models, because it can take into account CNT-CNT contact points that are Parallel and perpendicular to the CNT direction CNT-CNT contact With and without inter-CNT contact a Thermal boundary resistance R bd is calculated from Eq.1; epoxy density is 1.97 g/cm 3 [25]; epoxy specific heat is 0.97 J/gK [25] and sound velocity is 2400 m/s [26]. b f CN-CN is calculated from Eq.1; SWNT density is 1.3 g/cm 3 [22]; sound velocity in SWNTs is 8,000 m/s [23] and SWNT specific heat is 0.625 J/gK [24]. The same f CN-CN is assumed for the MWNTs due to unavailable experimental data.…”
Section: Discussionmentioning
confidence: 99%
“…Our TRIM simulation for irradiation of a bulk target indicates that a 30-keV Ar + ion transfers 800 eV/ion/nm to carbon atoms lying between the surface and a depth of 20 nm. For a (10,10) nanotube, and using [28] c v = 600 J/kg K for the specific heat of SWNTs, this means that an Ar + ion would heat a 13-nm portion of a nanotube to a temperature of 500 • C. Such temperatures are sufficient to cause substantial annealing of defects and desorption of adsorbed impurities. It is clear that propagation of heat further into the sample (beyond the stopping range of the ions) would raise temperatures sufficiently for annealing effects considerably deeper than the penetration depth of the ions, depending on the heat conductivity and other factors.…”
mentioning
confidence: 99%