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Journal of Spectroscopy
Volume 2013 (2013), Article ID 167357, 6 pages
http://dx.doi.org/10.1155/2013/167357
Research Article

Impact of Thermal Annealing under Nitrogen Ambient on Structural, Micro-Raman, and Thermogravimetric Analyses of Camphoric-CNT

1Centre of Nanoscience and Nanotechnology (NANO-SciTech Centre), Institute of Science, Universiti Teknologi MARA, Selangor, 40450 Shah Alam, Malaysia
2School of Physics and Material Studies, Faculty of Applied Sciences, Universiti Teknologi MARA, Selangor, 40450 Shah Alam, Malaysia
3Department of Physics, Faculty of Sciences and Mathematics, Universiti Pendidikan Sultan Idris, Perak, 35900 Tanjung Malim, Malaysia
4NANO-ElecTronic Centre, Faculty of Electrical Engineering, Universiti Teknologi MARA, Selangor, 40450 Shah Alam, Malaysia

Received 23 June 2012; Accepted 3 August 2012

Academic Editor: Roberto Flammini

Copyright © 2013 M. S. Shamsudin et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract

A systematical study of the effects on thermal annealing treatment under nitrogen ambient on the structural, micro-Raman, and thermogravimetric analyses of camphoric-carbon nanotubes (CNT) has been undertaken. Heat treatment of camphoric-CNT under nitrogen ambient was found to be an efficient technique of removing noncrystalline carbon and residual transition metal. Based on structural analysis, the heat-treated samples showed a clear view of overall camphoric-CNT structure.

1. Introduction

Over the last two decades, the official birth date of carbon nanotubes (CNT) was attributed to Japanese microscopist named Sumio Iijima. He was considered a “father of CNT” at that time affiliated at NEC Corporation, Japan, perished in a paper which shows his effort on the first discovery and remarkable potential of a new class of nano-structured carbon material [1]. It is important to notice that a common type of CNT is single-walled CNT (SWCNT) [2] and multiwalled CNT (MWCNT) [3] which can be visualized as a single and concentrically rolled-up sheet/s of graphene, respectively. CNT has gained great interests due to its superior intrinsic properties in terms of high thermal conductivity [4, 5], excellent mechanical strength [6, 7], and effective field emission characteristics [8, 9] suggesting their applicability for energy storage and conversion [10], filler in polymer nanocomposites [11], and flat-panel display [12]. There are several methods to eliminate the impurities in the as-synthesized CNT, including microwave digestion and radiation [13], reflux in acidic medium [14], and ultrasonication [15].

In the present paper, among the various purification techniques, we adopted thermal annealing treatment under nitrogen ambient coupled with different thermal annealing time by single-stage catalytic chemical vapor deposition (CVD) method. The effect of thermal annealing treatment time under nitrogen ambient on structural, micro-Raman, and thermogravimetric analysis was investigated. It demonstrated that nonoxidative gas-phase purification involves the elimination processes of some organometallic and carbonaceous particles from nanotubes. However, few effective methods have been reported for the removal of as-synthesized impurities, such as amorphous carbon (a-C) and catalyst without damaging the camphoric-CNT structure. Finally, this finding describes the removal-mechanism in terms of the strong relation between non-oxidative gas seniority upon exposure to form heat-treated camphoric-CNT was sought.

2. Experimental Description

2.1. Sample Preparation

In this study, camphoric-CNT was grown using two-stage catalytic CVD apparatus [16]. The processing and experimental setup/apparatus of as-synthesized camphoric-CNT were described elsewhere [17]. The optimized condition of 10% w/v (weight-volume percentage) of ferrocene relative to camphor oil was placed in different alumina boats. The alumina boats were positioned side by side along the quartz tube in the first furnace of two-stage catalytic CVD apparatus. The pretreatment of the evaporated camphor oil and sublimated ferrocene occur at 180°C at first furnace. The growth phase lasted for one hour at 800°C [18]. After the completion of growth phase, the first and second furnaces were shut down until room temperature was reached under constant cooling rate and then was ready for thermal annealing process.

The synthesized camphoric-CNT was then transferred to the thermal annealing system as can be seen in Figure 1. At first, each time, 0.5 g of synthesized camphoric-CNT was loaded into the system. The thermal annealing time was determined to fix the thermal annealing temperature. During the thermal annealing experiment, the system was kept at about 450°C in a lower flow rate of nitrogen (~10 sccm) and the thermal annealing times were changed from 2 to 10 minutes with 2-minute interval. Finally, at the same time, the mechanism of the thermal annealing process of each camphoric-CNT was discussed. In order to compensate such a drawback, as the time proceeds, it is hoped that more camphoric-CNT were exposed to the graphitic layer and have more chances to be attacked by the nitrogen molecules.

167357.fig.001
Figure 1: Schematic diagram of the apparatus that used for thermal annealing system.
2.2. Characterization Techniques

The surface morphology and structural behaviors of as-synthesized and annealed camphoric-CNT were characterized comprehensively using a field emission scanning electron microscope (FESEM, JEOL JSM-7600F) operated at 10 kV electron high tension (EHT) and 200 kX magnification. The degree of defect and graphitization of each sample was observed by a micro-Raman spectrometer (μ-Raman, HORIBA JOBIN HR800 Lab-Ram System) equipped with a 514.532 nm wavelengths Ar+ laser excitation as the light source. The power of the laser was adjusted by optical filter with a 100X objective lens. The μ-Raman spectra were recorded from 100 to 2000 cm−1. The thermogravimetric analysis was performed by thermogravimetric analyzer (TG, Perkin Elmer Pyris 1 TGA), operating at temperatures range from room temperature to 1000°C at a heating rate of 20°C/min in nitrogen ambient. The yield of camphoric-CNT before and after thermal annealing was determined.

3. Result and Discussion

3.1. Surface Morphology

The FESEM micrographs which analyzed the variation of as-synthesized and annealed (2, 4, 6, 8, and 10 minutes thermal annealing procedure) camphoric-CNT surface structures were shown in the Figure 2. In addition, the size of camphoric-CNT was determined and compared before and after a heat treatment process. From Figure 2(a), it is clear that as-synthesized camphoric-CNT has large-diameter ranges from 49.1 to 57.3 nm. The CNT diameter was slightly decreased to 51.4 nm as the thermal annealing was for 2 minutes as in Figure 2(b). As the time annealing increases further (from 4 to 6 minutes) the tube’s diameter was further decreased to smaller diameter range (26.7 to 22.1 nm). However, further increase in thermal annealing time (from 8 to 10 minutes) did not show any significant changes in tube’s diameter.

fig2
Figure 2: Typical FESEM images of the camphoric-CNT annealed at different thermal annealing time with 450°C thermal annealing temperature: (a) as-synthesized, (b) 2, (c) 4, (d) 6, (e) 8, and (f) 10 minutes.

The modification of the surface structure towards smoother morphology was also confirmed. Figure 2(a) showed the originality of camphoric-CNT, where the surface structure looks rough, uneven with bulge-like structure. These were believed due to a-C which was deposited on the tube wall. However, after the thermal annealing procedures were done, the reductions of tube’s diameter were clearly observed. Moreover, rough and uneven surfaces with a bulge still remain as shown in Figure 2(b). This shows that within 2-minute times of thermal annealing, procedures were not sufficient to eliminate the impurities that produced during the synthesis process. This suggested that all contaminant compounds and other impurities (i.e., a-C and byproduct carbon) were completely burnt off at 6-minute times without any camphoric-CNT structure collapse. We found that the smallest tube’s diameter was obtained at 6 minutes of thermal annealing time. However, the smoother and impurities-free surface was spotted at annealing time as shown in Figures 2(d) and 2(f), respectively. This study emphatically proves that by reordering the carbon structure, the sample is almost free from a-C layer in which tube wall produces relatively hollow and bright inside. As confirmed by FESEM micrograph as in Figure 2(f), the dense camphoric-CNT is completely transformed to translucent camphoric-CNT (marked with red circle). It is found that when they overlapped, we could see another transparent (see-through) CNT-2 behind CNT-1.

We are not matured enough to understand the principle of a removal mechanism of the world inside nanotubes unless by providing specialized laboratory equipment, we will be able to do insitu measurement. There are many basic issues and highly debatable questions concerning the removal mechanism awaiting solid answers to fulfill expectations [19]. However, it is hard to visualize the crucial role of nitrogen atmosphere in removal-mechanism of camphoric-CNT. It is important to note that under these theoretical assumptions and experimental verifications, is discussed below:(i)To elucidate this, consider the relationship of kinetic energy and motion in gas phase. At a lower temperature (−273.15°C), the particles of nitrogen (constituent of molecules) have no kinetic energy, in which the molecules are as closely as possible in complete rest, and it defines two things: (a) nitrogen molecules have minimal motion and (b) they maintain only quantum-mechanical motion [20]. Though nitrogen is considered as nearly inert gas. However, at higher temperature (~450°C), nitrogen molecules can react with carbon material as thermal annealing treatment time increased. It seems more reasonable to associate the thermal annealing treatment to the nature of kinetic energy nitrogen gas. It is a certain kind of vibrational motion of its constituent nitrogen molecules called translational motion in gas. As expected, nitrogen molecules move in three-dimensional space (-, -, and -axis). It means that the nitrogen molecules move in spatial degrees of freedom. We believe that a-C layer were placed and stuck together on the outer layer of camphoric-CNT. There are several points of support in the above-mentioned removal mechanism. It is speculated that nitrogen molecules behave as a oxidizing agent and a-C will be etched layer by layer by nitrogen molecules as thermal annealing treatment time increased. (ii)Besides, nitrogen molecules act as a carrier agent. Since a-C layer has low thermal stability at a higher temperature compared to perfect ideal CNT [21]. This phenomenon could happen due to a-C layer sublimates at 450°C. After that, a-C layer can be directly purged out from the single-stage thermal annealing system by nitrogen gas.

3.2. Micro-Raman Analysis

The degree of graphitization and crystal camphoric-CNT structure can be analyzed by micro-Raman spectroscopy at room temperature. Figures 3(a) and 3(b) show the micro-Raman spectra of as-synthesized and annealed camphoric-CNT using a 514.532 nm wavelengths Ar+ laser excitation in the wavenumber range from 100 to 500 cm−1 and 1000 to 2000 cm−1 [22, 23], respectively. Figure 3(a) shows that the normalized radial breath mode (RBM) at the lower frequency region of small tubes is sensitive to the tube diameter and valid in the range of 0.5 < < 2.48 nm. By using Bandon’s equation [24], the diameter of SWCNT can be evaluated from normalized intensity of RBM peak’s position , as = 248 (nmcm−1)/ (cm−1). While for large tubes, the effect of tube diameter on the normalized RBM frequency is ignorable, this might be due to the existence of MWCNT. As shown in Figure 3(b), we can see the deconvolution spectrum of tangential mode (TM) located at (i) 1380 cm−1 assigned to the disorder-induced phonon mode (D-band) and (ii) 1600 cm−1 designated C–C stretching graphitic mode (G-band) [25]. In particular interest, the narrowing of the bands is the evaluation of the ratio. The lower ratio corresponds for better crystallinity of graphitic structure [26]. The improvement of the intensity ratio is proven by the appearance of defects in the as-synthesized camphoric-CNT which decreased due to defect reduction process as the thermal annealing treatment time increased.

fig3
Figure 3: Micro-Raman spectra of camphoric-CNT grown by two-stage catalytic CVD at different thermal annealing time for the following: (a) RBM and (b) TM. Positions of (*) and peaks are shown.

According to this study, the effect of thermal annealing treatment time under nitrogen ambient can be interpreted by using micro-Raman analysis. At the band area of RBM, no peaks related to SWCNT were observed for as-synthesized, 2- and 4-minute treated camphoric-CNT samples. The peaks of SWCNT appear at 6-, 8-, and 10-minute treated camphoric-CNT. The positions of were located at 214.4 and 278.4 cm−1 for 6 minutes, 234.4 and 293.0 cm−1 for 8 minutes, and 250.4 and 315.7 cm−1 for 10 minutes. From micro-Raman analysis, the calculated values of were summarized as in Table 1. The number of walls and diameter in MWCNT can be estimated by an empirical law and quickly determined using FESEM, if the nanotubes are individually distinguishable, which is suggested by Chiodarelli et al. [27]. There are many conflicting reports since the perfect ideal CNT is far from the practically producing CNT today. However, this theory is valid if the CNT is free from any contaminants (i.e., metal catalyst and a-C layer) and structural defect.

tab1
Table 1: Tabulated data of and ratio for as-synthesized and at different thermal annealing treatment time using micro-Raman analysis.

As shown in Figure 3(b) and Table 1, there is a gradual trend of decreas ratio as thermal annealing treatment time increased. Moreover, it is confirmed from the micro-Raman analysis that the lowest ratio is 0.442 at 10 minutes ofthermal annealing treatment time. Thus, the thermal annealing treatment time under nitrogen ambient has efficiently enhanced the removal of the structural defects.

3.3. Thermogravimetric Analysis

Normally, TG analysis is a part of quantitative determination to define the purity of CNT. In this study, the TG analysis was performed in the oxygen ambient, while the temperature increases at rate of 20°C/min. For every sample, TG analysis was done up to 1000°C to evaluate thermal stability and purity of as-synthesized and annealed camphoric-CNT. A plot of the weight loss monitoring thermal stability of camphoric-CNT in weight changes of the sample (including camphoric-CNT, metal catalyst, and impurities) versus temperature has been shown in Figure 4. From this diagram, it is seen that 68.01, 94.71, 96.75, 98.98, 99.17, and 99.75% of the total weight came from C element for as-synthesized, 2, 4, 6, 8, and 10 minutes of thermal annealing treatment time samples. It is found that camphoric-CNT for all samples is completely burned around 600°C. The residual mass is the mass that was left due to orange-like powder in the sample pan at the end of the characterization process. The lowest residual iron catalyst was found to be 0.25% at 10 of minutes thermal annealing treatment time.

167357.fig.004
Figure 4: Graph of TG-analysis of camphoric-CNT for the as-synthesized, 2, 4, 6, 8, and 10 of minutes thermal annealing time.

4. Conclusion

The influence of thermal annealing under nitrogen ambient on structural, micro-Raman, and TG analyses of as-synthesized and annealed camphoric-CNT has been examined in to thermal annealing process; thermal annealing treatment time is the critical parameter that determines length and diameter distribution, disordered and graphitic feature, and percentage yield of camphoric-CNT. It is evaluated that the texture of camphoric-CNT changed according to the thermal annealing treatment time, by FESEM observation. Since the thermal annealing treatment time decreased the ID/IG ratio of the camphoric-CNT, it also has a significant effect of graphitization degree. However, the defects in the nanotubes structure still remained but reduced in quantity; the enhancement of graphitization degree leads to a greater thermal stability that is shown in TG analysis. TG curves showed the camphoric-CNT had highest percentage yield ~99.75% at 10 minutes thermal annealing treatment time. As a result, in order to produce camphoric-CNT of well-defined properties in mass production, it is advisable that further investigations required to understand the world inside nanotubes.

Acknowledgments

One of the authors (M. S. Shamsudin) is grateful to Universiti Teknologi MARA through Graduate Service Scheme and Excellence Fund (under Contact no. 600-RMI/DANA 5/3/Dst (435/2011)) for financial supports. The authors also would like to thank the Malaysian Ministry of Higher Education for providing (it is MyMaster scholarship program). Thanks are due to NANO-SciTech Centre and NANO-ElecTronic Centre colleagues for valuable technical assistance. The authors acknowledge the constructive comments from anonymous reviewers.

References

  1. S. Iijima, “Helical microtubules of graphitic carbon,” Nature, vol. 354, no. 6348, pp. 56–58, 1991. View at Google Scholar · View at Scopus
  2. S. Iijima and T. Ichihashi, “Single-shell carbon nanotubes of 1-nm diameter,” Nature, vol. 363, no. 6430, pp. 603–605, 1993. View at Google Scholar · View at Scopus
  3. Z. Sadeghian, “Large-scale production of multi-walled carbon nanotubes by low-cost spray pyrolysis of hexane,” New Carbon Materials, vol. 24, no. 1, pp. 33–38, 2009. View at Publisher · View at Google Scholar · View at Scopus
  4. H. Xie, A. Cai, and X. Wang, “Thermal diffusivity and conductivity of multiwalled carbon nanotube arrays,” Physics Letters, Section A, vol. 369, no. 1-2, pp. 120–123, 2007. View at Publisher · View at Google Scholar · View at Scopus
  5. D. J. Yang, S. G. Wang, Q. Zhang, P. J. Sellin, and G. Chen, “Thermal and electrical transport in multi-walled carbon nanotubes,” Physics Letters, Section A, vol. 329, no. 3, pp. 207–213, 2004. View at Publisher · View at Google Scholar · View at Scopus
  6. H. Rafii-Tabar, “Computational modelling of thermo-mechanical and transport properties of carbon nanotubes,” Physics Reports, vol. 390, no. 4-5, pp. 235–452, 2004. View at Publisher · View at Google Scholar · View at Scopus
  7. R. B. Pipes and P. Hubert, “Helical carbon nanotube arrays: mechanical properties,” Composites Science and Technology, vol. 62, no. 3, pp. 419–428, 2002. View at Publisher · View at Google Scholar · View at Scopus
  8. A. Mayer and P. Lambin, “Quantum-mechanical simulations of field emission from carbon nanotubes,” Carbon, vol. 40, no. 3, pp. 429–436, 2002. View at Publisher · View at Google Scholar · View at Scopus
  9. A. L. Musatov, N. A. Kiselev, D. N. Zakharov et al., “Field electron emission from nanotube carbon layers grown by CVD process,” Applied Surface Science, vol. 183, no. 1-2, pp. 111–119, 2001. View at Publisher · View at Google Scholar · View at Scopus
  10. S. L. Candelaria, Y. Shao, W. Zhou et al., “Nanostructured carbon for energy storage and conversion,” Nano Energy, vol. 1, no. 2, pp. 195–220, 2012. View at Publisher · View at Google Scholar · View at Scopus
  11. H. Zhang and Z. Zhang, “Impact behaviour of polypropylene filled with multi-walled carbon nanotubes,” European Polymer Journal, vol. 43, no. 8, pp. 3197–3207, 2007. View at Publisher · View at Google Scholar · View at Scopus
  12. Y. Saito and S. Uemura, “Field emission from carbon nanotubes and its application to electron sources,” Carbon, vol. 38, no. 2, pp. 169–182, 2000. View at Publisher · View at Google Scholar · View at Scopus
  13. C.-M. Chen, M. Chen, F.-C. Leu et al., “Purification of multi-walled carbon nanotubes by microwave digestion method,” Diamond and Related Materials, vol. 13, no. 4-8, pp. 1182–1186, 2004. View at Publisher · View at Google Scholar · View at Scopus
  14. K. L. Strong, D. P. Anderson, K. Lafdi, and J. N. Kuhn, “Purification process for single-wall carbon nanotubes,” Carbon, vol. 41, no. 8, pp. 1477–1488, 2003. View at Publisher · View at Google Scholar · View at Scopus
  15. D. A. Heller, P. W. Barone, and M. S. Strano, “Sonication-induced changes in chiral distribution: a complication in the use of single-walled carbon nanotube fluorescence for determining species distribution,” Carbon, vol. 43, no. 3, pp. 651–653, 2005. View at Publisher · View at Google Scholar · View at Scopus
  16. M. S. Shamsudin, M. F. Achoi, M. N. Asiah et al., “An investigation on the formation of carbon nanotubes by two-stage chemical vapor deposition,” Journal of Nanomaterials, vol. 2012, Article ID 972126, 5 pages, 2012. View at Publisher · View at Google Scholar · View at Scopus
  17. M. S. Shamsudin, S. Abdullah, and M. Rusop, “Structural and thermal behaviors of iron-filled align carbon nanotubes formulated by two-stage catalytic chemical vapor deposition,” Advanced Materials Research, vol. 364, pp. 191–195, 2012. View at Publisher · View at Google Scholar · View at Scopus
  18. M. S. Shamsudin, N. A. Asli, S. Abdullah, S. Y. S. Yahya, and M. Rusop, “Effect of synthesis temperature on the growth iron-filled carbon nanotubes as evidenced by structural, micro-Raman, and thermogravimetric analyses,” Advances in Condensed Matter Physics, vol. 2012, Article ID 420619, 7 pages, 2012. View at Publisher · View at Google Scholar
  19. E. F. Antunes, V. G. De Resende, U. A. Mengui, J. B. M. Cunha, E. J. Corat, and M. Massi, “Analyses of residual iron in carbon nanotubes produced by camphor/ferrocene pyrolysis and purified by high temperature annealing,” Applied Surface Science, vol. 257, no. 18, pp. 8038–8043, 2011. View at Publisher · View at Google Scholar · View at Scopus
  20. J. McKenna and H. L. Frisch, “Quantum mechanical microscopic Brownian motion,” Physics Letters, vol. 19, no. 2, pp. 112–114, 1965. View at Google Scholar · View at Scopus
  21. D. R. Tallant, J. E. Parmeter, M. P. Siegal, and R. L. Simpson, “The thermal stability of diamond-like carbon,” Diamond and Related Materials, vol. 4, no. 3, pp. 191–199, 1995. View at Google Scholar · View at Scopus
  22. Y. Ouyang and Y. Fang, “A new surface-enhanced Raman scattering system for carbon nanotubes,” Spectrochimica Acta. Part A, vol. 61, no. 9, pp. 2211–2213, 2005. View at Publisher · View at Google Scholar · View at Scopus
  23. L. Lafi, D. Cossement, and R. Chahine, “Raman spectroscopy and nitrogen vapour adsorption for the study of structural changes during purification of single-wall carbon nanotubes,” Carbon, vol. 43, no. 7, pp. 1347–1357, 2005. View at Publisher · View at Google Scholar · View at Scopus
  24. M. Aydin and D. L. Akins, “Calculated dependence of vibrational band frequencies of single-walled and double-walled carbon nanotubes on diameter,” Vibrational Spectroscopy, vol. 53, no. 1, pp. 163–172, 2010. View at Publisher · View at Google Scholar · View at Scopus
  25. N. Bendiab, R. Almairac, M. Paillet, and J. L. Sauvajol, “About the profile of the tangential modes in single-wall carbon nanotube bundles,” Chemical Physics Letters, vol. 372, no. 1-2, pp. 210–215, 2003. View at Publisher · View at Google Scholar · View at Scopus
  26. S. Kawasaki, M. Shinoda, T. Shimada, F. Okino, and H. Touhara, “Single-walled carbon nanotubes grown on natural minerals,” Carbon, vol. 44, no. 11, pp. 2139–2141, 2006. View at Publisher · View at Google Scholar · View at Scopus
  27. N. Chiodarelli, O. Richard, H. Bender et al., “Correlation between number of walls and diameter in multiwall carbon nanotubes grown by chemical vapor deposition,” Carbon, vol. 50, no. 5, pp. 1748–1752, 2012. View at Publisher · View at Google Scholar · View at Scopus