Journal of Nanomaterials
Volume 2016 (2016), Article ID 4942398, 8 pages
http://dx.doi.org/10.1155/2016/4942398

Research Article

Investigations of Electron Properties of Carbon Nanotubes Decorated with Platinum Nanoparticles with Their Varying Fraction

Anna Dobrzańska-Danikiewicz,¹ Dariusz Łukowiec,¹ and Jerzy Kubacki2,3

¹Faculty of Mechanical Engineering, Silesian University of Technology, Konarskiego 18a Street, 44-100 Gliwice, Poland
²Silesian Center for Education and Interdisciplinary Research, 75 Pułku Piechoty 1A, 41-500 Chorzów, Poland
³A. Chełkowski Institute of Physics, University of Silesia, Uniwersytecka 4, 40-007 Katowice, Poland

Received 10 January 2016; Accepted 2 March 2016

Academic Editor: Hassan Karimi-Maleh

Copyright © 2016 Anna Dobrzańska-Danikiewicz 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.

The paper presents the outcomes of investigations into electron properties and a qualitative and quantitative analysis of the chemical composition of unmodified carbon nanotubes with comparison to nanotubes decorated with platinum nanoparticles. The fabricated nanocomposite materials of the CNT-Pt type differed in a varying mass concentration of platinum nanoparticles (5, 10, and 20% of Pt). X-ray photoelectron spectroscopy (XPS) was employed to examine the structure and to analyse chemical composition. Survey spectra measurements within a wide range of the binding energy of 0–1400 eV were performed in the first phase of the investigations. The core lines of C1s carbon, Pt4f platinum, and O1s oxygen and a valence band were then measured. The chemical composition of the studied materials was determined based on the measured spectra of the core lines. The purpose of the investigations is to determine the effect of platinum nanoparticles on the structure and electron properties of the fabricated CNT-Pt nanocomposites.

1. Introduction

The principal task imposed on the present and future generations of engineers is to design and fabricate new materials with unique properties. The requirements that engineering materials must satisfy these days become out of date very rapidly due to efforts to achieve better and better functional characteristics of the products fabricated with such materials. The discovery of carbon nanotubes in 1991 has launched a series of intensive studies into this new allotrope type of carbon, confirming their unique mechanical, electrical, thermal, and optical properties [1–4]. Carbon nanotubes are characterised by a large specific area and high electrical conductivity. Moreover, they are chemically stable, elastic, resistant to bending, stretching, and torsion, and also lightweight [5–7]. Their density—depending on the type—ranges over 0.6–2.6 g/cm³ [8, 9]. A broad spectrum of nanotubes’ uncommon properties indicates their substantial application opportunities as independent materials or components of material systems. Scientists are especially interested in nanotubes because of their chemical modification, which opens up utterly new application vistas for nanotubes. This new branch of investigations into nanotubes encompasses molecular surface sorption, attachment of function groups to their surface and endings, improved wettability, and also the additions of other elements outside, inside, and within a graphene nanotube plane. The chemical functionalisation of carbon nanotubes enables developing completely new composite materials combining the unique properties of nanotubes and other materials, where it becomes possible to control their electrical, mechanical, thermal, and optical properties [10–15]. The results of own research and the research pursued by research institutions [16–23] confirm that deposition of nanoparticles of noble metals such as Pd, Pt, Rh, and Au onto a surface of carbon nanotubes may contribute to a substantially higher density of carriers of free loads and hence to nanotubes’ enhanced thermal and electrical conductivity. A practical application of the so developed nanotubes-nanoparticles type materials is sensors of selected chemical substances, including H₂, CH₄, and NO₂ [24]. The key advantages of sensors containing active material in the form of a CNT-Pt composite are high chemical and thermal resistance, no requirement to work at an elevated temperature, as in a majority of optional solutions, operating sensitivity, fast reaction, and selectivity.

This paper presents the results of investigations into the structure and electron properties of CNT-Pt type nanocomposite materials with a varying mass fraction of platinum nanoparticles.

2. Experimental

Multiwalled carbon nanotubes with the length of 100–200 μm and diameter of 10–20 nm fabricated with the Chemical Vapour Deposition (CVD) technique were employed for investigations whose aim was to recognise the electron properties of the fabricated nanocomposite materials (Figure 1). 8% chloroplatinic acid, H₂PtCl₆, supplied by Sigma-Aldrich (USA) was used for synthesising the platinum nanoparticles.

Figure 1: SEM and TEM images of multiwalled carbon nanotubes used in the investigations [37].

Three sets of specimens containing, respectively, 5, 10, and 20% of platinum nanoparticles deposited on the surface of carbon nanotubes were prepared for spectroscopic studies (Figure 2). CNT-Pt type nanocomposites were prepared by the preliminary treatment of the surface of carbon nanotubes with function groups (–COOH, –COH, and =CO) through their covalent functionalisation in a mixture of acids. Platinum nanoparticles were synthesised by way of chemical reduction in the second phase of the process, and then they were deposited onto the surface of nanotubes. A methodology of carbon nanotubes’ functionalisation and decoration with platinum nanoparticles was already detailed in the authors’ earlier works [19, 24]. The investigations of physiochemical properties together with a qualitative and quantitative analysis of chemical composition of unmodified carbon nanotubes and CNT-Pt type nanocomposites were performed with X-ray photoelectron spectroscopy (XPS) using a PHI 5700/660 photoelectron spectrometer by Physical Electronics. Monochromatic X-ray radiation coming from an Al Kα aluminium anode with the radiation energy of  eV was used to carry out the measurements. The energy resolution of the spectrometer used for the tests was 0.3 eV.

(a)

(b)

(c)

Figure 2: TEM photographs of CNT-Pt nanocomposites with varying fraction of Pt nanoparticles: (a) CNT-5% Pt, (b) CNT-10% Pt, and (c) CNT-20% Pt [37].

The material intended for the tests was deposited directly onto the surface of a PREVAC PTS STANDARD specimen carrier and placed in an XPS measuring chamber. Survey spectra were measured, within a wide range of binding energy of 0–1400 eV. The core lines of C1s carbon, Pt4f platinum, and O1s oxygen and a valence band were then measured. The measurements were made in a high-resolution mode with pass energy of 23.5 eV. The chemical composition of the studied materials was determined on the basis of the measured spectra of core lines and MultiPak software was used for chemical composition calculations [25]. The shape of the core lines was determined with the Voigt profile containing a compound Doniach-Sunjic function [26–28]. The Shirley function was used for determination of background lines [29, 30].

3. Results and Discussion

Figure 3 shows a review spectrum created as a result of examining unmodified carbon nanotubes with X-ray photoelectron spectroscopy excited with X-ray photoelectron spectroscopy. Two main photoemission lines are shown on the spectrum for which the maximum counts for the binding energy of 285 eV and 533 eV correspond, respectively, to electron states of carbon marked as C1s and oxygen marked as O1s. Carbon content in the nanotube material was identified at the level of 98.7% in atomic terms, while oxygen content is 1.3% in atomic terms. A small amount of the adsorbed oxygen, as compared to the amount of carbon, signifies a good quality of the studied material. Figure 4 shows the measured core lines for the states C1s and O1s obtained in a high-resolution mode. The performed profile analysis of the lines reveals a complex character of carbon lines (Figure 4(a)). A spectrum shape of the C1s line exhibits the presence of three components. The binding energy of the particular components is, respectively, 284.2 eV, 284.4 eV, and 285.9 eV. The energy location of the profile lines corresponds to carbon states with the hybridisation sp² and sp³ in a carbon nanotube [31]. The third component is probably connected with the presence of carbon in the adsorbed CO molecules on the surface of nanotubes [31] or with manufacturing conditions. The O1s line (Figure 4(b)) consists of only one component with the binding energy of about 533 eV. The binding energy of the oxygen line corresponds to OH groups [32]. A wide line for energy above 1200 eV, visible in Figure 3, corresponds to Auger electron emission as a result of passing between KLL levels for carbon.

Figure 3: XPS spectrum of unmodified carbon nanotubes.

(a)

(b)

Figure 4: Spectra of C1s and O1s core lines obtained in high-resolution mode: (a) deconvolution of C1s line and (b) O1s photoemission line.

Figure 5 presents a valence band achieved for the studied nanotube material. A valence band obtained from the surface of Highly Oriented Pyrolytic Graphite (HOPG) was added for reference. The maximum photoemission of the valence band occurs in both cases for the binding energy of approx. 18.5 eV. An additional feature is visible on the spectrum for both measured specimens at the energy of about 13.5 eV. The third characteristic feature, less visible for CNT material, exists for the binding energy of about 8 eV. A shape of a valence band of CNT material is therefore reflecting a hexagonal structure of carbon bonds in graphite. An interesting valence band area, presenting the electron states related to the existence of π-type and σ-type bonds between carbon atoms in a nanotube, occurs in the binding energy area below 10 eV. The same type of bonds exists also in the electron structure of graphite [33].

Figure 5: Valence band of unmodified nanotubes of CNT and graphite HOPG.

Figures 6, 7, and 8 show the results of photoemission measurements of carbon nanotubes modified with platinum nanoparticles (CNT-5% Pt, CNT-10% Pt, and CNT-20% Pt), obtained in a wide range of binding energy. Photoemission lines are visible on the spectra coming from the states of core lines of C1s carbon (about 284 eV), O1s oxygen (about 531 eV), Auger C KLL lines (approx. 1200 eV), and O KLL lines (about 980 eV). Photoemission lines of 4p, 4d, and 4f platinum are visible in the form of doublets related to the spin-orbit interaction. Photoemission lines related to the states of fluorine, F1s, and sodium, Na1s, occur additionally on the spectrum created for the CNT-10% Pt specimen. Depending on the mass fraction of platinum (5, 10, and 20%) in the newly created nanocomposites, the intensity of photoemission lines for electron states 4p, 4d, 4f, and 5p of platinum is growing.

Figure 6: XPS spectrum of carbon nanotubes modified with CNT-5% Pt platinum nanoparticles.

Figure 7: XPS spectrum of carbon nanotubes modified with CNT-10% Pt platinum nanoparticles.

Figure 8: XPS spectrum of carbon nanotubes modified with CNT-20% Pt platinum nanoparticles.

Figure 9 presents C1s photoemission lines achieved for carbon nanotubes modified with platinum nanoparticles as compared to unmodified nanotubes. Similarly to an unmodified CNT material, a profile analysis of a C1s core line of specimens enriched with platinum was undertaken. Similarly to the input material, the presence of components corresponding to sp³ and sp² hybridisation was demonstrated. A negligible increase in the intensity of the sp² component and a decrease in the intensity of the sp³ component were seen in the modified material versus the CNT input material. The ratio of bonds between carbon atoms, determined for a material modified with platinum nanoparticles according to variations in intensities of sp³ and sp² components, is not changing. It can therefore be assumed that an increased concentration of platinum in the modified material is not substantially changing the number of sp³ and sp² bonds in carbon nanotubes.

(a)

(b)

(c)

(d)

Figure 9: Spectra of C1s core line for (a) unmodified carbon nanotubes (CNT) and nanotubes modified with platinum nanoparticles for their varied mass fraction, including (b) CNT-5% Pt, (c) CNT-10% Pt, and (d) CNT-20% Pt.

Figure 10 shows the 4f core lines of platinum obtained for carbon nanotubes modified with platinum nanoparticles with their varying fraction (5, 10, and 20% by mass of Pt). The structure of the measured 4f states consists of two 4f7/2 and 4f5/2 lines connected with spin-orbit interaction, creating a so-called doublet. A detailed profile analysis has shown the presence of two doublets which moved in relation to each other by 3.3 eV. The first doublet for the binding energy of 71.2 eV for the state 4f7/2 corresponds to the presence of platinum in a metallic state, while the other doublet for the binding energy of 74.5 eV for the state 45/2 is connected with platinum oxide PtO₂ [31, 34–36]. It is apparent from Figure 10 that the intensity of the doublet 45/2 is rising as the percentage fraction of platinum is growing.

(a)

(b)

(c)

Figure 10: Spectra of Pt4f core line for carbon nanotubes modified with platinum nanoparticles for their varied fraction, including (a) CNT-5% Pt, (b) CNT-10% Pt, and (c) CNT-20% Pt.

Figure 11 shows the measured core lines for the states O1s of oxygen obtained in a high-resolution mode. The performed profile analysis of the lines reveals a complex character of O1s lines (Figures 11 and 12). A spectrum shape exhibits the presence of five components. The binding energy of the oxygen line component of 530.2 eV corresponds to platinum oxide PtO₂ (platinum with the 4th level of oxidisation of PtO₂). When analysing the intensity of the oxygen line component of 530.2 eV together with a varying mass fraction of platinum of, respectively, 0, 5, 10, and 20% of Pt, growth for this value can be seen (Figure 11). This phenomenon confirms the growth of the platinum oxide, PtO₂, fraction in the analysed materials along with a varying fraction of nanoparticles (5, 10, and 20% by mass of Pt). The energy location of the successive components of the line O1s is shown in Figure 12. The additional oxygen line components signify the presence of oxygen compounds created in the process of carbon nanotubes’ modification with platinum.

(a)

(b)

(c)

Figure 11: Spectra of O1s core line for carbon nanotubes modified with platinum nanoparticles for their varied fraction: (a) CNT-5% Pt, (b) CNT-10% Pt, and (c) CNT-20% Pt.

Figure 12: Location of O1s line components for carbon nanotubes modified with platinum nanoparticles (CNT-5% Pt).

Figure 13 presents the structure of a valence band of CNT material with a varied degree of modification with platinum nanoparticles as compared to the band of unmodified nanotubes and HOPG graphite. A shape of a valence band for graphite (HOPG) in the lower part of the figure was added for reference. A shape of a valence band of CNT material is therefore similar to HOPG and reflects a hexagonal structure of carbon bonds in graphite. The modification of carbon nanotubes with platinum nanoparticles will deliver 5d platinum electrons to a valence band structure of the nanotubes. Figure 13 allows observing an increase in the photoemission of 5d electrons of platinum depending on the modification degree of the nanotubes with platinum nanoparticles. The investigations carried out with a standard source of XPS radiation do not allow pointing out variations in the character of π and σ bonds in the analysed materials, due to a high density of 5d state of platinum.

Figure 13: Structure of valence band area of carbon nanotubes modified with platinum nanoparticles for their varied fraction of CNT-5% Pt, CNT-10% Pt, and CNT-20% Pt against unmodified nanotubes and graphite.

A quantitative chemical composition analysis confirms the higher contents of platinum in the studied nanocomposites along with its varying mass fraction (Table 1). A CNT-5% Pt specimen features the concentration of carbon, oxygen, and platinum with the following concentrations: C (90.9% at.), O₂ (8.2% at.), and Pt (0.9% at.). The chemical composition of the CNT-10% Pt specimen is as follows: C, 90.4% at., O₂, 7.7% at., and Pt, 1.9% at.; and, according to the initial assumptions, platinum content in the analysed materials grows two times (1.9% at.). A twofold growth of platinum content of 3.8% at. compared to the CNT-10% Pt specimen was recorded for the CNT-20% Pt nanocomposite with the following % at. composition: C, 86.5%, O₂, 9.7%, and Pt, 3.8%.

Table 1: Quantitative chemical composition analysis of unmodified carbon nanotubes and nanocomposites with varying fraction of platinum (CNT-5% Pt, CNT-10% Pt, and CNT-20% Pt).

Material
C (% at.)
O₂ (% at.)
Pt (% at.)
Na (% at.)
F (% at.)

Unmodified CNTs
98.7
1.3
—
—
—

CNT-5% Pt
90.9
8.2
0.9
—
—

CNT-10% Pt
90.4
7.7
1.9
<1
<1

CNT-20% Pt
86.5
9.7
3.8
—
—

4. Conclusion

The results of photoemission measurements (XPS) obtained for the nanocomposites have shown the presence of photoemission lines in the spectra coming from the states of core lines of C1s carbon, O1s oxygen, and 4p, 4d, and 4f platinum, which are visible in the form of doublets related to the spin-orbit interaction. As the mass fraction of platinum nanoparticles (5, 10, and 20%) in a CNT-Pt nanocomposite is rising, the intensity of photoemission lines for the electron states 4p, 4d, and 4f of platinum is rising. A profile analysis of a core line C1s of the input material and of this modified with platinum nanoparticles shows the presence of components corresponding to sp³ and sp² carbon hybridisation. It has been confirmed on the basis of the investigations performed that an increased concentration of platinum in the modified material is not substantially changing the number of sp³ and sp² bonds in carbon nanotubes. The modification of carbon nanotubes with platinum nanoparticles delivers, however, 5d platinum electrons to a valence band structure of the nanotubes, which is manifested by a higher density of electron states at the Fermi surface.

Competing Interests

The authors declare that they have no competing interests.

Acknowledgments

The paper was financed from a statutory grant of the Faculty of Mechanical Engineering of the Silesian University of Technology in 2015 in the framework of 10/990/BK_15/0013 project. The scientific experiments have been made within the framework of the ELCONANO project headed by Professor Anna Dobrzańska-Danikiewicz, funded by the Polish National Science Centre in the framework of the “OPUS” competitions. The project was awarded a subsidy under the decision DEC-2011/03/B/ST8/06070.

References

S. Iijima, “Helical microtubules of graphitic carbon,” Nature, vol. 354, no. 6348, pp. 56–58, 1991.

P. M. Ajayan, “Nanotubes from carbon,” Chemical Reviews, vol. 99, no. 7, pp. 1787–1799, 1999.

T. W. Ebbesen, H. J. Lezec, H. Hiura, J. W. Bennett, H. F. Ghaemi, and T. Thio, “Electrical conductivity of individual carbon nanotubes,” Nature, vol. 382, no. 6586, pp. 54–56, 1996.

C. Journet and P. Bernier, “Production of carbon nanotubes,” Applied Physics A: Materials Science & Processing, vol. 67, no. 1, pp. 1–9, 1998.

M. Meyyappan, Carbon Nanotubes. Science and Application, CRC Press LLC, Boca Raton, Fla, USA, 2005.

M. M. J. Treacy, T. W. Ebbesen, and J. M. Gibson, “Exceptionally high Young's modulus observed for individual carbon nanotubes,” Nature, vol. 381, no. 6584, pp. 678–680, 1996.

S. Frank, P. Poncharal, Z. L. Wang, and W. A. de Heer, “Carbon nanotube quantum resistors,” Science, vol. 280, no. 5370, pp. 1744–1746, 1998.

S. M. Mukhopadhyay, Ed., Nanoscale Multifunctional Materials: Science and Applications, John Wiley & Sons, Hoboken, NJ, USA, 2012.

X. Zhang, H. Ju, and J. Wang, Electrochemical Sensors, Biosensors and Their Biomedical Applications, Elsevier, San Diego, Calif, USA, 2008.

V. Georgakilas, D. Gournis, V. Tzitzios, L. Pasquato, D. M. Guldi, and M. Prato, “Decorating carbon nanotubes with metal or semiconductor nanoparticles,” Journal of Materials Chemistry, vol. 17, no. 26, pp. 2679–2694, 2007.

X. Peng, J. Chen, J. A. Misewich, and S. S. Wong, “Carbon nanotube-nanocrystal heterostructures,” Chemical Society Reviews, vol. 38, no. 4, pp. 1076–1098, 2009.

G. G. Wildgoose, C. E. Banks, and R. G. Compton, “Metal nanoparticles and related materials supported on carbon nanotubes, methods and applications,” Small, vol. 2, no. 2, pp. 182–193, 2006.

A. D. Dobrzańska-Danikiewicz, D. Łukowiec, D. Cichocki, and W. Wolany, “Carbon nanotubes decorating methods,” Archives of Materials Science and Engineering, vol. 61, no. 2, pp. 53–61, 2013.

A. M. Rao, P. C. Eklund, S. Bandow, A. Thess, and R. E. Smalley, “Evidence for charge transfer in doped carbon nanotube bundles from raman scattering,” Nature, vol. 388, no. 6639, pp. 257–259, 1997.

R. S. Lee, H. J. Kim, J. E. Fischer, A. Thess, and R. E. Smalley, “Conductivity enhancement in single-walled carbon nanotube bundles doped with K and Br,” Nature, vol. 388, no. 6639, pp. 255–257, 1997.

A. Star, V. Joshi, S. Skarupo, D. Thomas, and J.-C. P. Gabriel, “Gas sensor array based on metal-decorated carbon nanotubes,” Journal of Physical Chemistry B, vol. 110, no. 42, pp. 21014–21020, 2006.

A. Jorio, M. S. Dresselhaus, and G. Dresselhaus, Carbon Nanotubes. Advanced Topics in the Synthesis, Structure, Properties and Applications, vol. 111 of Topics in Applied Physics, Springer, Berlin, Germany, 2008.

A. D. Dobrzańska-Danikiewicz, D. Łukowiec, and D. Cichocki, “The MWCNTs-Rh nanocomposite obtained by the new high-temperature method,” Archives of Metallurgy and Materials, vol. 60, no. 2, pp. 1057–1063, 2015.

A. D. Dobrzańska-Danikiewicz and D. Lukowiec, “Synthesis and characterization of Pt/MWCNTs nanocomposites,” Physica Status Solidi (B) Basic Research, vol. 250, no. 12, pp. 2569–2574, 2013.

A. D. Dobrzańska-Danikiewicz, D. Łukowiec, D. Cichocki, and W. Wolany, “Comparison of the MWCNTs-Rh and MWCNTs-Re carbon-metal nanocomposites obtained in high-temperature,” Archives of Metallurgy and Materials, vol. 60, no. 3, pp. 2053–2060, 2015.

A. D. Dobrzańska-Danikiewicz, D. Cichocki, and D. Łukowiec, “Obtaining and description of the MWCNTs-Pd nanocomposite,” Archives of Materials Science and Engineering, vol. 74, no. 1, pp. 15–22, 2015.

K. Lee, J. Zhang, H. Wang, and D. P. Wilkinson, “Progress in the synthesis of carbon nanotube- and nanofiber-supported Pt electrocatalysts for PEM fuel cell catalysis,” Journal of Applied Electrochemistry, vol. 36, no. 5, pp. 507–522, 2006.

Y. Xing, “Synthesis and electrochemical characterization of uniformly-dispersed high loading Pt nanoparticles on sonochemically-treated carbon nanotubes,” Journal of Physical Chemistry B, vol. 108, no. 50, pp. 19255–19259, 2004.

A. D. Dobrzańska-Danikiewicz, M. Procek, D. Łukowiec, T. Gaweł, and M. Procek, “Resistance changes of carbon nanotubes decorated with platinum nanoparticles in the presence of hydrogen at different and constant concentrations,” Physica Status Solidi (B), vol. 251, no. 12, pp. 2426–2431, 2014.

ULVAC-PHI, MultiPakTM Software,VERSION 9.6.1.7, Part No. 706704 Rev. D, ULVAC-PHI, Chigasaki, Japan, 2015.

R. Hesse, T. Chassé, and R. Szargan, “Peak shape analysis of core level photoelectron spectra using UNIFIT for WINDOWS,” Fresenius' Journal of Analytical Chemistry, vol. 365, no. 1–3, pp. 48–54, 1999.

S. Doniach and M. Sunjic, “Many-electron singularity in X-ray photoemission and X-ray line spectra from metals,” Journal of Physics C: Solid State Physics, vol. 3, no. 2, pp. 285–291, 1970.

S. Tougaard, “Quantitative XPS: non-destructive analysis of surface nano-structures,” Applied Surface Science, vol. 100-101, pp. 1–10, 1996.

J. E. Castle and A. M. Salvi, “Interpretation of the Shirley background in x-ray photoelectron spectroscopy analysis,” Journal of Vacuum Science & Technology A, vol. 19, no. 4, pp. 1170–1175, 2001.

D. A. Shirley, “High-resolution x-ray photoemission spectrum of the valence bands of gold,” Physical Review B, vol. 5, no. 12, pp. 4709–4714, 1972.

B. Ha and O. H. Han, “Platinum-catalyzed carbon nanotubes for durability enhancement of low-temperature fuel cells,” Journal of Power Sources, vol. 223, no. 1, pp. 246–253, 2013.

C. D. Wagner, D. A. Zatko, and R. H. Raymond, “Use of the oxygen KLL auger lines in identification of surface chemical states by electron spectroscopy for chemical analysis,” Analytical Chemistry, vol. 52, no. 9, pp. 1445–1451, 1980.

L. Fleming, M. D. Ulrich, K. Efimenko et al., “Near-edge absorption fine structure and UV photoemission spectroscopy studies of aligned single-walled carbon nanotubes on Si(100) substrates,” Journal of Vacuum Science and Technology B: Microelectronics and Nanometer Structures, vol. 22, no. 4, pp. 2000–2004, 2004.

C. R. Parkinson, M. Walker, and C. F. McConville, “Reaction of atomic oxygen with a Pt(1 1 1) surface: chemical and structural determination using XPS, CAICISS and LEED,” Surface Science, vol. 545, no. 1-2, pp. 19–33, 2003.

Z. Liu, X. Lin, J. Y. Lee, W. Zhang, M. Han, and L. M. Gan, “Preparation and characterization of platinum-based electrocatalysts on multiwalled carbon nanotubes for proton exchange membrane fuel cells,” Langmuir, vol. 18, no. 10, pp. 4054–4060, 2002.

F. Şen and G. Gökaǧaç, “Different sized platinum nanoparticles supported on carbon: an XPS study on these methanol oxidation catalysts,” Journal of Physical Chemistry C, vol. 111, no. 15, pp. 5715–5720, 2007.

D. Łukowiec, The structure and properties of nanocomposites composed of carbon nanotubes coated with platinum nanoparticles [Ph.D. thesis], Silesian University of Technology, Gliwice, Poland, 2014.