A versatile method for direct determination of iron content in multi-wall carbon nanotubes by inductively coupled plasma atomic emission spectrometry with slurry sample introduction

Joanna Bok-Baduraa, Agata Jakóbik-Kolon*a, Marian Tureka, Sławomir Boncelb and Krzysztof Karońc
aSilesian University of Technology, Faculty of Chemistry, Department of Inorganic, Analytical Chemistry and Electrochemistry, Bolesława Krzywoustego 6, 44-100 Gliwice, Poland. E-mail: agata.jakobik@polsl.pl; Tel: +48 322371990
bSilesian University of Technology, Faculty of Chemistry, Department of Organic Chemistry, Biochemistry and Biotechnology, Bolesława Krzywoustego 4, 44-100 Gliwice, Poland
cSilesian University of Technology, Faculty of Chemistry, Department of Physical Chemistry and Technology of Polymers, Marcina Strzody 9, 44-100 Gliwice, Poland

Received 23rd October 2015 , Accepted 19th November 2015

First published on 20th November 2015


Abstract

Carbon nanotubes (CNTs), due to their unique combination of physicochemical properties, are continuously considered as one of the most interesting materials in contemporary science and industry. Their applicability depends on physical properties, such as number of walls, morphology, diameter and length (aspect ratio), but also on the content of carbonaceous and metallic contaminants (typically present as encapsulated catalyst nanoparticles from catalytic Chemical Vapor Deposition). Therefore, especially for medical and biomedical applications, the concentration of metallic impurities or modifiers should be monitored. In this paper, an inductively coupled plasma atomic emission spectrometry (ICP-AES) technique with slurry nebulization is proposed for direct determination of iron in multi-wall carbon nanotubes (MWCNTs). Slurries of MWCNTs are prepared in a 1% solution of Triton X-100, ultrasonicated to ensure their homogeneity and measured by the ICP-AES apparatus. The optimal range of MWCNTs slurry concentration and plasma radiofrequency (RF) power are established as 40–500 mg L−1 and 1.0 kW, respectively. The precision of the method does not exceed 1.5% of the mean values. Validation of the method is based on the fact that Fe is partly leached from the slurry and the assumption that iron in the leachate gives the same response in ICP-AES as iron in the residual MWCNTs slurry. This behavior was proved by summing both results for Fe (determined in the leachate and in the slurry of post-leaching nanotubes), which always yielded the same total amount of Fe for different degrees of leaching and this value was in full agreement with the iron content in the original, tested sample, as determined by the proposed slurry method. Taking into account all the examinations and obtained results, it can be concluded that the proposed method is applicable for fast, versatile, direct, and simple quantitative analysis of iron in MWCNTs and potentially other nanoallotropes produced by c-CVD.


1. Introduction

Multi-wall carbon nanotubes (MWCNTs) due to their unique electrical, optical, magnetic and mechanical properties are one of the most interesting materials of the 21st century. CNTs have already been or will be in the forthcoming future applied in the following fields: electronics, power engineering, industrial catalysis, military technology or (broadly defined) materials engineering (filler in polymers, ceramic and metallic nanocomposites including heat- and electric conductors, high performance CNT fibers, nanoliquids, antifouling paints etc.)1 Currently, a great interest for carbon nanotubes (CNTs) in medicine and biotechnology (e.g. drugs or vaccine delivery systems, biomaterials and biosensors) is observed.2–4

Synthesis of MWCNTs – the most scalable and synthesized with low costs nanotubes – typically requires catalyst (Fe, Ni, Y, Co, Mo, La) which is essential in their high yield controllable growth and selective formation. However, the catalyst particles usually remain in the final product as encapsulated or to-CNT-wall tethered impurities which may fundamentally alter the nanotube properties (e.g. electronic, magnetic etc.). Moreover, these impurities may generate non-specific eco- and cytotoxicity to the produced material.3,5 On the other hand, in some cases metal nanoparticles may be introduced into/onto MWCNTs deliberately to achieve tunable properties (e.g. iron-enriched MWCNTs as contrast agent in magnetic resonance imaging or in targeted drug delivery systems).6 The presence of metal nanoparticles in CNTs, especially as for medical and biomedical application, should be fast and conveniently monitored to avoid changes of their properties. This statement is also true for industrial synthesis of MWCNTs where quality control and emissions levels will constitute key values for the market of nanomaterials and public health.

A lot of methods have been already proposed to examine structure, physical properties and chemical composition of MWCNTs including thermogravimetric analysis (TGA),7–9 Raman spectroscopy,7,8 transmission electron microscopy (TEM),7 scanning electron microscopy (SEM), scanning electron microscopy/energy dispersive X-ray spectrometry (SEM/EDX),3 transmission electron microscopy/energy dispersive X-ray spectrometry (TEM/EDX),10 X-ray photoelectron scattering,3 X-ray fluorescence11 or neutron activation analysis (NAA).12,13 Although these methods are commonly used, they have certain limitations e.g. TGA – the most popular method for determination the metal content in CNTs does not provide the information about the type of elements but only about the content of non-combustible and/or non-volatile part of sample.10,11 Other microscope methods like TEM, SEM, etc. are only surface sensitive and are insufficiently sensitive for determination of trace metal residues, particularly if the metal is encapsulated in core of individual CNTs. Generally, most of these methods are applicable for qualitative or semi-quantitative analyses, whereas the information about chemistry of impurities or modifier content are either unavailable or can be only estimated. NAA is the most appropriate technique for determination of metal content in CNTs, but it is not widely used due to the fact that the nuclear reactor is required.3 In other methods like inductively coupled plasma atomic emission spectrometry (ICP-AES) or inductively coupled plasma mass spectrometry (ICP-MS), which could give full information on concentration of particular elements, liquid samples are required.13 Due to the extreme difficulties in digesting/dissolving pristine CNTs, the procedures of preparation of liquid samples constitute the most important as well as the most problematic step in the whole process of analysis. Dry ashing and dissolution in concentrated nitric acid, wet acid digestion, microwave-assisted digestion or microwave induced combustion digestion were proposed to prepare samples to ICP-AES or ICP-MS.3,5,14 Unfortunately, these methods are often time-consuming, laborious, multistage, and not always give a complete digestion which may cause erroneous results in the further analysis.10 Furthermore, for dry ashing large amounts of sample must be used and, for this reason, this method cannot be used in a small laboratory scale. These methods also require the use of aggressive chemicals and conditions (e.g. for microwave-assisted dissolution procedure the mixture of nitric and perchloric acid must be applied) and depend on the type and structure of materials.14 The alternative method for digestion of CNTs and subsequent determination of total iron requires using a mixture of 70% HNO3 and 90% H2SO4 (1[thin space (1/6-em)]:[thin space (1/6-em)]1, v/v) and 17 h of reflux.15 This method is time consuming and preparation of a large number of samples would be difficult.

Therefore, direct, fast and simple analytical method for quantitative analysis of metal modifiers or metal impurities in CNTs is necessary. In this work, we propose fast and simple analytical method for direct determination of total iron content in MWCNTs using ICP-AES with a slurry sample introduction. This method has been previously used successfully for determination of elements in various materials (e.g. coal, titanium dioxide, dolomite and magnesia, cement etc.).16–19 Importantly, it is straightforward to implement and does not require modification of the ICP-AES equipment.

2. Experimental

2.1. Apparatus

Determination of iron concentration was performed utilizing Varian 710-ES spectrometer equipped with a V-groove nebulizer and a reduced-volume Sturman–Masters type spray chamber made of poly(tetrafluorethylene) (Varian). The operating parameters and the selected analytical lines were presented in Table 1. For determination of slurry concentration UV-VIS spectrophotometer (Varian, Carry 50 Scan) was used. The absorbance at the wavelength of 500 nm in a 1 cm glass cuvette was measured. SEM (Scanning electron microscope – Phenom Pro Desktop SEM) was used to obtain the micrographs of MWCNTs. EA (Elemental Analysis, Perkin Elmer 2400 Series II CHNS/O analyzer) to obtain an approximate values of iron content were utilized. For mineralization the MARS 5 CEM Corp. was used (200 °C, ramp time 15 min, hold time 15 min).
Table 1 The operating parameters of ICP-AES analysis
Parameter Value
RF power, kW 1.0
Ar plasma flow rate, L min−1 15
Ar carrier flow rate, L min−1 1.5
Nebulizer pressure, kPa 210
Pump rate, rpm 15
Viewing Axial
Fe wavelength, nm 234.350, 261.187, 261.382


2.2. Materials and reagents

MWCNTs used in this study were synthesized by c-CVD (Chemical Vapor Deposition) according to a procedure previously described (760 °C, FeCp2 – ferrocene, bis(η5-cyclopentadienyl)iron as iron precursor, toluene as carbon source and Ar as carrier gas).20 Preliminary characterization of this material was performed using SEM, whereas for estimation of the total iron concentration in pristine (as-synthesized) MWCNTs elemental analysis (EA) was used. Triton X-100 – surfactant (Sigma-Aldrich) and nitric acid (65%, Suprapur, Merck) were used to prepare the slurries. All of the slurries, dispersions and solutions were prepared using ultrapure water (MilliporeElix 10 System).

2.3. Concentration of MWCNTs in the slurries – UV-VIS analysis

A few slurry samples of various MWCNT concentration in 1% Triton X-100 aqueous solution were prepared for calibration. Blank solution was also prepared (1% Triton X-100) and used as the reference. On the basis on calibration curve, the actual concentrations of MWCNTs in the slurries were computed in the further experiments.

2.4. ICP-AES analysis

2.4.1. Calibration. Calibration curves for ICP-AES analysis were established with standard solution of Fe (CPI International, 1 mg mL−1 in 2% HNO3) in 1% Triton X-100 and 5% HNO3. In order to prove the impact of the presence of Triton X-100 in the samples on the obtained results, the calibration curves without this dispersant were also prepared. The results were computed as an average values from the calibration curves in the range of 0.1–25 mg L−1 obtained from 3 used analytical lines (Table 1).
2.4.2. Sample preparation. Primary slurry samples of MWCNTs were prepared by weighting appropriate amount of nanotubes and further ultrasonication (ultrasonic bath Bandelin Sonorex RK 106, 35 kHz, 480 W, 80 °C) in the solution of 1% Triton X-100 and 5% nitric acid for 15 min to ensure homogeneity. Triton X-100 was selected as a dispersing agent, on the basis on previously described experiments.4,21
2.4.3. Effect of slurry concentration on determination of iron. The primary slurry sample was next properly diluted to obtain slurries of various concentrations of MWCNTs in the range of 2 to 500 mg L−1. The actual concentrations of MWCNTs in the obtained slurries were determined by the UV-VIS analysis. The concentration of total iron in the prepared slurries was measured by ICP-AES applying parameters provided in Table 1. The results were computed as mean values from the calibration curves obtained from 3 analytical lines. For each slurry concentration, six parallel samples were prepared and the final result was calculated as the mean value.
2.4.4. Effect of plasma power on determination of iron content. To examine the effect of RF power (plasma power) on determination of iron in the studied nanotubes, samples – prepared as described above – were measured applying various RF power (1.0, 1.2, 1.4 kW). The concentration of iron in the slurries were measured by ICP-AES applying condition provided in Table 1 except for 1.4 kW plasma power where higher plasma and carrier gas flow rates were applied (16.5 and 1.7 L min−1 respectively). The results were computed as mean values obtained from 3 analytical lines using the calibration curves measured under given conditions. The final result was calculated as average value from six parallel samples.

2.5. Evaluation of the slurry method

The elaborated here slurry method was applied since MWCNTs used in these studies could not be completely digested – obtaining clear solution was impossible. Due to the lack of the certified reference materials similar to tested sample, validation of the method was based on the fact that Fe is partly leached from the slurry and assumption that iron in the leachate gives the same response in ICP-AES as iron in the residual MWCNTs slurry so the same calibration as for Fe in solution must work correctly also for Fe in the slurry. Therefore in order to test the proposed slurry method, iron was leached from iron-containing CNTs sample by two different methods: (1) leaching with the solution of 5% nitric acid and 1% Triton X-100; (2) microwave-assisted leaching with a mixture of concentrated acids (HNO3 and H2SO4, 4[thin space (1/6-em)]:[thin space (1/6-em)]1). The amount of iron in the leachate was determined by ICP-AES method. The post-leaching MWCNTs was filtered, washed, and used for the preparation of slurry. Because it was impossible to quantitatively transfer MWCNTs from the filter, the concentration of the prepared slurry was determined by UV-VIS method. The iron content in the slurry prepared from the post-leaching MWCNTs was determined using the proposed slurry method. Subsequently, the sum of iron content in the leachate and iron content in post-leaching CNTs was compared with the iron content determined in the investigated material by the evaluated slurry method.

3. Results and discussion

3.1. MWCNT characterization

Micromorphology of the examined material was observed using SEM (Fig. 1A and B). In addition, SEM micrographs were used to indicate effectiveness of dispersion of MWCNTs in Triton X-100 solutions (Fig. 1C). In the original material, long, needle-like, aligned fibrous nanotubes covered with a few catalyst nanoparticles visible as brighter spots were observed. In turn, after dispersion, the nanotubes were found as distributed randomly. Differences in the appearance of slurries after the sonication could be observed with an unarmed eye – (Fig. 2A and B). Elemental analysis showed 95.5% ± 0.4% of carbon, 0.0% of nitrogen and 0.0% of hydrogen in the sample. Assuming that residual part of the sample was iron, ca. 4% of total iron was estimated in studied nanotube sample.
image file: c5ra22269a-f1.tif
Fig. 1 SEM micrographs of MWCNTs: (A), (B) original; (C) after dispersion in Triton X-100 solution.

image file: c5ra22269a-f2.tif
Fig. 2 Slurries of MWCNTs in 1% Triton X-100: (A) before ultrasonication; (B) after ultrasonication.

3.2. Concentration of MWCNTs in the slurries – UV-VIS analysis

The calibration curve prepared in the range of 0 to 160 mg L−1 slurry concentration (Fig. 3) fulfilled the Lambert–Beer–Bouger Law and was used to examine the actual concentration of MWCNT in the slurries intended for further experiments.
image file: c5ra22269a-f3.tif
Fig. 3 UV-VIS calibration curve for measurement the MWCNT concentration in the slurries.

3.3. ICP-AES analysis

3.3.1. Calibration. In order to ensure homogeneity of the slurry, a dispersing agent should be introduced to the mixture.4,22 For this purpose, Triton X-100 was selected on the basis on previously described experiments. The benzene ring present in the Triton X-100 chemical structure indicates that this non-ionic compound could be a good surfactant for dispersion of MWCNTs.4,20 However, each additional substance may produce matrix effects during the ICP-AES measurements. Therefore, the impact of Triton X-100 (used as surfactant) on iron analytical signal was examined. For this purpose the calibration curves with and without Triton X-100 were prepared (Fig. 4). The signals obtained without Triton X-100 were of the lower intensity than those obtained for the samples with Triton X-100. These outcomes proved that the presence of Triton X-100 was mandatory also for preparation the calibration standards to avoid false results.
image file: c5ra22269a-f4.tif
Fig. 4 The effect of Triton X-100 presence in the standards for determination of iron on analytical signal intensity (λFe = 234.350 nm).
3.3.2. Sample preparation. To avoid errors caused by weighting small amounts of samples, slurries from a larger amount of MWCNT sample were prepared and, next, they were diluted to obtain slurries of desired MWCNT concentrations. The actual MWCNT concentrations in the obtained slurries were determined by UV-VIS analysis and they were consistent with the established values. In addition, this protocol proved the appropriate selection of homogenization procedure (dispersing agent as well as ultrasonication conditions).
3.3.3. Effect of MWCNT concentration in the slurry on determination of the total iron content in MWCNTs. Concentration of MWCNTs in the slurry may have a significant impact on its analysis caused by quality of dispersion, atomization and transportation of the slurry to the plasma and also excitation efficiency into plasma.22,23 Therefore, the effect of MWCNT concentration in the slurry on determination of total iron content was investigated (Fig. 5). Statistical test (t-Student's) showed no significant difference for the results measured using slurries of MWCNT concentration in the range 40–500 mg L−1, a slight deterioration of the results for 10–20 mg L−1 and significant deterioration for 2 mg L−1. This significant decrease in the measured values may be caused by a too low number of individual MWCNTs to form homogenous slurry. This behavior may be also connected with poor precision, evaluated as expanded uncertainty by calculating the confidence interval (95% confidence level, 6 replicates). In this case, the confidence interval was ca. 10%. For determination of iron using other slurry concentrations (10–500 mg L−1), the precision of the method was fully reliable and did not exceed 2%. Taking into account the good precision as well as no significant difference between results measured in range of concentration of 40 to 500 mg L−1 MWCNTs in the slurry, further research should be performed in this range. These examinations and the results from the combustion elemental analysis allowed us also to establish the reference value of iron in the studied material as 3.64 ± 0.05%. Obviously, the best route to validate the method would be to use the certified reference material (CRM), unfortunately, the CRM of MWCNTs for determination of iron have not been available yet, mainly due to a broad spectrum of synthetic protocols and a variety of nanotube morphologies.
image file: c5ra22269a-f5.tif
Fig. 5 Effect of the MWCNT concentration in the slurry on iron determination of total iron content in pristine MWCNTs.
3.3.4. Effect of plasma power on iron determination. The RF power may change the temperature of the plasma and alternate the population of the excited atoms. Increasing the RF power increases the quantity of the excited atoms and the radiation emission which is directly related with the intensity of the analytical signals. The maximum RF power at which the ICP-AES instrument utilized in this study can work was 1.4 kW. However, to save the generator lifetime, the lowest RF power is preferred for the routine work. Therefore, the effect of RF power have been determined at plasma power 1.0, 1.2 and 1.4 kW. The results from determination of the iron content in the MWCNT samples are presented in Fig. 6. In addition, various concentrations of MWCNTs in the slurry were taken into consideration.
image file: c5ra22269a-f6.tif
Fig. 6 Effect of the RF power used for determination iron in the MWCNT slurries at various concentrations.

Generally, there was no statistically significant difference between results for a given slurry concentration measured in the investigated plasma power range. Increasing plasma power did not extend the working range of slurry concentration. As mentioned previously, at the lowest utilized slurry concentrations (2 mg L−1, 10 mg L−1), the obtained values were underestimated. The underestimation was also observed in the case of 1.4 kW plasma power and at the highest MWCNT concentration in the slurry. We can only speculate that during the excitation in plasma, short-lived Fe–C compounds can be created at the highest temperature (easier to exceed activation energies of formation reactions) and at the highest MWCNT concentration (high Fe–C collision frequency). Those molecular species have completely different emission and absorption spectra from “pure” Fe and C atoms, and thus if the atomization of iron is not complete it would result in lowering of the Fe concentration.

Since, no significant influence of RF power to measurement results was observed in the further research, 1.0 kW plasma power could be used as the optimal value.

3.4. Evaluation of the analytical method

Preliminary studies showed that even mineralization in a closed system using microwaves and a mixture of concentrated acids (HNO3 and H2SO4, 4[thin space (1/6-em)]:[thin space (1/6-em)]1, v/v) did not digest the investigated nanotubes. After so-performed mineralization a lot of thick, black, floccose precipitate was still present in the mixtures. Hence, it was impossible to completely digest MWCNTs in order to directly determine the iron content in nanotubes. In addition, there are neither certified reference materials for MWCNTs nor for iron in any type of CNTs. Therefore, to test the proposed slurry method, iron was leached from iron-containing MWCNT sample using two procedures. In case of leaching with the solution of 5% nitric acid and 1% Triton X-100, less iron was transferred to the leachate (35–42%) than in the case of microwave-assisted leaching with a mixture of concentrated nitric and sulfuric acids (84–97%) – Tables 2 and 3. Also, the difference in iron content determined in the slurry prepared from the post-leaching CNTs was observed – in the first procedure: 57–64%, in the second: 2–14%. In both of these cases the iron leaching took place, but in case of microwave-assisted leaching with mixture of concentrated acids was more efficient. Unfortunately, contrary to the first case, the results of leaching were unrepeatable. The results proved that under the examined conditions, the complete leaching of iron was impossible and the use of the slurry method was necessary. To prove the correctness of iron determination in the CNTs slurry, results of a total amount of iron (determined in leachate and in slurry of post-leaching nanotubes) and the reference value were compared. The comparison showed that the sum of iron content in the leachate and iron content in post-leaching MWCNTs, calculated for different degrees of leaching, was in full agreement with the iron content in the original, tested sample, as determined by the proposed slurry method. Those comparative studies proved our assumption that iron in the leachate gives the same response in ICP-AES as iron in the residual MWCNTs slurry was justified and correct. Therefore the same calibration as for Fe in solution could be employed also for Fe in the slurry and the results obtained by the slurry method was assumed to be correct.
Table 2 Mass balance of iron in leaching studies (leaching medium – 5% HNO3 and 1% Triton X-100)
  Amount of iron leached from 1 g of CNTs [mg] (A) Mass contribution of iron determined in leachate to the total iron mass [%] (B) Amount of iron in 1 g of CNTs after leaching [mg] (C) Mass contribution of iron determined in solid residue to the total iron mass [%] (D) Total amount of iron in 1 g of CNTs, sum of (A) and (C) [mg] (E) Amount of iron in 1 g of original CNTs determined by slurry sampling [mg] (F) Recovery (E) × 100/(F) [%]
1 13.6 37.57 22.6 62.43 36.2 36.4 102.1
2 15.6 42.13 21.4 57.87 36.9 98.6
3 13.1 35.11 24.2 64.89 37.3 102.3


Table 3 Mass balance of iron in the leaching studies (microwave-assisted leaching with conc. HNO3 and H2SO4)
  Amount of iron leached from 1 g of CNTs [mg] (A) Mass contribution of iron determined in leachate to the total iron mass [%] (B) Amount of iron in 1 g of CNTs after leaching [mg] (C) Mass contribution of iron determined in solid residue to the total iron mass [%] (D) Total amount of iron in 1 g of CNTs, sum of (A) and (C) [mg] (E) Amount of iron in 1 g of original CNTs determined by slurry sampling [mg] (F) Recovery (E) × 100/(F) [%]
1 35.94 97.76 0.82 2.24 36.76 36.4 101.12
2 34.37 95.91 1.47 4.09 35.83 98.57
3 31.45 84.03 5.98 15.97 37.43 102.96


3.5. Determination of iron in MWCNTs by the slurry sampling ICP-AES technique

Based on the previously described experiment, the optimal parameters for the MWCNT slurry sample preparation and for determination of iron in MWCNTs were established.

Ten 0.1 mgL−1 MWCNT samples were ultrasonicated for 1 h in 1% Triton X-100 solution. Next, they were measured under conditions provided in Experimental section. The results are presented in Table 4. The calculated mean value of iron content in the investigated MWCNTs was in agreement with the above-established actual value. Precision of the method, evaluated as expanded uncertainty by calculating the confidence interval (95% confidence level, 10 replicates), was high and did not exceed 1.5% of the mean value. These outcomes constitute the evidence that the proposed method of determination of total iron content in MWCNTs by the slurry sampling ICP-AES technique is fully applicable.

Table 4 Repeatability of iron determination in MWCNTs by evaluated method (u – confidence interval at 95% confidence level, 10 replicates)
No. of sample Iron concentration [%]
1 3.70
2 3.71
3 3.77
4 3.68
5 3.58
6 3.56
7 3.70
8 3.65
9 3.65
10 3.62
Mean value 3.66
u 0.05


4. Conclusions

In this study, a fast, simple and versatile ICP-AES technique with slurry sample nebulization for direct iron determination in MWCNTs was presented. The influence of slurry concentration and the RF power on iron determination were examined. Generally, no significant effect of either RF power in the range of 1.0–1.4 kW or MWCNT concentration in the slurry in the range of 40–500 mg L−1 was observed. Based on those results, the iron concentration in the examined MWCNTs was established as 3.64 ± 0.05%. Precision of the proposed method was high, and did not exceed 1.5% of mean value. Using the proposed ICP-AES technique with the slurry sampling avoids the laborious, time-consuming sample preparation steps. Therefore, the proposed method may be a rapid, economic, more environmental-friendly and extensible to numerous carbon- and non-carbon nanomaterials way for direct determination of total iron content.

Acknowledgements

S. Boncel thanks the National Science Centre in Poland (program SONATA, 2012/05/D/ST5/03519) the Foundation for Polish Science (39/UD/SKILLS/2015, ‘Impuls’ program) and National Science Centre & The National Centre for Research and Development (program TANGO1, TANGO1/266702/NCBR/2015), all Poland, for the financial support.

Notes and references

  1. M. F. L. de Volder, S. H. Tawfick, R. H. Baughman and A. J. Hart, Science, 2013, 339, 535–539 CrossRef CAS PubMed.
  2. Y. Lin, S. Taylor, H. Li, K. A. S. Fernando, L. Qu, W. Wang, L. Gu, B. Zhou and Y.-P. Sun, J. Mater. Chem., 2004, 14, 527 RSC.
  3. C. Ge, F. Lao, W. Li, Y. Li, C. Chen, Y. Qiu, X. Mao, B. Li, Z. Chai and Y. Zhao, Anal. Chem., 2008, 80, 9426–9434 CrossRef CAS PubMed.
  4. R. Rastogi, R. Kaushal, S. K. Tripathi, A. L. Sharma, I. Kaur and L. M. Bharadwaj, J. Colloid Interface Sci., 2008, 328, 421–428 CrossRef CAS PubMed.
  5. L. Ayouni-Derouiche, M. Méjean, P. Gay, M.-L. Milliand, P. Lantéri, L. Gauthier and E. Flahaut, Carbon, 2014, 80, 59–67 CrossRef CAS.
  6. N. Kuźnik, M. M. Tomczyk, S. Boncel, A. P. Herman, K. K. K. Koziol and M. Kempka, Mater. Lett., 2014, 136, 34–36 CrossRef.
  7. C. M. Chen, M. Chen, Y.-W. Peng, H.-W. Yu and C.-F. Chen, Thin Solid Films, 2006, 498, 202–205 CrossRef CAS.
  8. K. L. Strong, D. P. Anderson, K. Lafdi and J. N. Kuhn, Carbon, 2003, 41, 1477–1488 CrossRef CAS.
  9. S. Scaccia, M. Carewska and P. P. Prosini, Thermochim. Acta, 2005, 435, 209–212 CrossRef CAS.
  10. T. Kolodiazhnyi and M. Pumera, Small, 2008, 4, 1476–1484 CrossRef CAS PubMed.
  11. B. Cavness, J. Heimbecker, J. Velasquez and S. Williams, Radiat. Phys. Chem., 2012, 81, 131–134 CrossRef CAS.
  12. T. Braun, H. Rausch, L. P. Bíró, Z. Konya and I. Kiricsi, J. Radioanal. Nucl. Chem., 2004, 262, 31–34 CrossRef CAS.
  13. R. Zeisler, R. L. Paul, R. Oflaz Spatz, L. L. Yu, J. L. Mann, W. R. Kelly, B. E. Lang, S. D. Leigh and J. Fagan, Anal. Bioanal. Chem., 2011, 399, 509–517 CrossRef CAS PubMed.
  14. P. A. Mello, L. F. Rodrigues, M. A. G. Nunes and J. C. P. Mattos, Instrumentation, 2011, 22, 1040–1049 CAS.
  15. S. Boncel and K. K. K. Koziol, Appl. Surf. Sci., 2014, 301, 488–491 CrossRef CAS.
  16. M. Mujuru, R. I. McCrindle, B. M. Botha and P. P. Ndibewu, Fuel, 2009, 88, 719–724 CrossRef CAS.
  17. Z. Wang, Z. Ni, D. Qiu, T. Chen, G. Tao and P. Yang, J. Anal. At. Spectrom., 2004, 19, 273 RSC.
  18. J. Bok-Badura, A. Jakóbik-Kolon, M. Turek, J. Szczerba, M. Lemanowicz and K. Karoń, Spectrochim. Acta, Part B, 2015, 113, 79–83 CrossRef CAS.
  19. L. Marjanovic, R. I. McCrindle, B. M. Botha and J. Hermanus Potgieter, J. Anal. At. Spectrom., 2000, 15, 983–985 RSC.
  20. S. Boncel, K. K. K. Koziol, K. Z. Walczak, A. H. Windle and M. S. P. Shaffer, Mater. Lett., 2011, 65, 2299–2303 CrossRef CAS.
  21. P. Randhawa, J.-S. Park, S. Sharma, P. Kumar, M.-S. Shin and S. S. Sekhon, J. Nanoelectron. Optoelectron., 2012, 7, 279–286 CrossRef CAS.
  22. L. Ebdon, M. Foulkes and K. Sutton, J. Anal. At. Spectrom., 1997, 12, 213–229 RSC.
  23. M. Henryk, in Advances in Atomic Spectroscopy, 2002, vol. 7, pp. 237–248 Search PubMed.

This journal is © The Royal Society of Chemistry 2015