Thermal degradation of ragged single-wall carbon nanotubes produced by polymer-assisted ultrasonication

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Abstract

As-grown single-wall carbon nanotubes (SWNTs) and a monochlorobenzene (MCB) solution of polymethylmethacrylate (PMMA) were sonicated using an ultrasonic processor. The SWNTs obtained were short and contained many holes and defects; therefore, they were called `ragged single-wall carbon nanotubes (r-SWNTs)'. The r-SWNTs were degraded at and above 800°C in a vacuum (10−7 Torr). All the r-SWNTs disappeared after heat-treatment at 1200°C for 1 h. Since thermal degradation was not observed for as-grown SWNTs or for acid-purified SWNTs, we suggest that the holes and defects in the r-SWNTs were formed by oxidation of chemically damaged sites formed during the polymer-assisted ultrasonication.

Introduction

Since the discovery of single-wall carbon nanotubes (SWNTs) [1] their nature, including their structure, and electronic and mechanical properties, has been revealed as a result of many investigations. However, many impurities, such as amorphous carbon, fullerenes, and metal catalysts, are produced together with SWNTs. High-quality SWNTs need to be produced to study the detailed bulk properties of SWNTs and to develop applications for their use. Some methods for purifying SWNTs have been reported. Carbonaceous impurities can be removed by gas-phase oxidation [2], and metal impurities can be eliminated using a strong acid, followed by filtration and centrifugation [3].

The separation of SWNTs and impurities is more difficult than general separation techniques, largely because SWNTs of various lengths form bundles, to which impurities adhere. Ultrasonic irradiation is one effective method for dispersing, disentangling, and thinning bundles of SWNTs when SWNTs are purified. Smalley and co-workers [4] reported purifying and cutting SWNTs by ultrasonically assisted filtration. Recently, our group has reported that ultrasonication and filtration of a mixture of SWNTs and polymethylmethacrylate (PMMA) was a more effective method for removing carbonaceous impurities, and we also found a number of short SWNTs (about 1 μm) and thin bundles containing one to three SWNTs [5].

In this study, we found that SWNTs purified by polymer-assisted ultrasonication had worm-eaten-like holes and they rapidly sublimed at temperatures over 800°C. These were named `ragged SWNTs (r-SWNTs)'. Here we report the first successful observation of the degradation of SWNTs and the characterization of r-SWNTs.

Section snippets

Experimental

SWNTs were produced by a conventional laser ablation method. A pellet (diameter 10mm×5mm) was prepared as the laser target by compressing powdered graphite containing metal catalysts, Co and Ni, with atomic concentrations of 0.6% each. The second harmonic output of an Nd:YAG laser (532 nm, 10 Hz, 6–7 ns, 0.7 J/pulse, Spectra Physics GCR-350) was used to ablate the Ni/Co/graphite target at a temperature of 1200°C in an Ar flow (750 Torr, 300 ml/min).

Approximately 5 mg of the as-grown SWNTs and

Results and discussion

As-grown SWNTs contained impurities, such as metal particles, carbonaceous particles, and amorphous carbons (Fig. 1a); the impurities adhered to the surface of bundles of SWNTs. Most of the as-grown SWNTs formed arch-like bundles. The inset in Fig. 1a indicates that most of the bundles contained about 50 SWNTs with diameters of ca. 1.3 nm.

Fig. 1b shows a TEM image of SWNTs (US) obtained by ultrasonication followed by filtration through 5 μm pores. SWNTs (US) were not clearly observed by TEM, as

Conclusions

In this study, we found that r-SWNTs were produced by polymer (PMMA)-assisted ultrasonication and oxidation. We have also observed their unusual property of thermal degradation by heat treatment in a vacuum. The degradation occurs at temperatures exceeding 800°C. We suggest that the holes and defects in the r-SWNTs are formed by oxidation at sites damaged by the polymer-assisted ultrasonication, and that these sites are the starting point for the degradation. The instability and reactivity of

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