DOI:
10.1039/C4RA00469H
(Paper)
RSC Adv., 2014,
4, 13742-13748
Rhodium(0) nanoparticles supported on nanotitania as highly active catalyst in hydrogen generation from the hydrolysis of ammonia borane
Received
16th January 2014
, Accepted 31st January 2014
First published on 4th February 2014
Abstract
Rhodium(0) nanoparticles supported on the surface of titanium dioxide (Rh(0)@TiO2) were in situ generated from the reduction of rhodium(III) ions impregnated on nanotitania during the hydrolysis of ammonia borane. They were isolated from the reaction solution by centrifugation and characterized by a combination of advanced analytical techniques. The results show that (i) highly dispersed rhodium(0) nanoparticles with sizes in the range 1.3–3.8 nm were formed on the surface of titanium dioxide, (ii) Rh(0)@TiO2 shows high catalytic activity in hydrogen generation from the hydrolysis of ammonia borane with a turnover frequency value up to 260 min−1 at 25.0 ± 0.1 °C, (iii) the results of kinetic studies on the hydrogen generation from the hydrolysis of ammonia borane were also reported including the activation energy of 65.5 ± 2 kJ mol−1 for this reaction.
Introduction
Ammonia-borane (NH3BH3, AB) has been regarded as one of the leading candidates for hydrogen storage materials for on-board hydrogen applications due to its high hydrogen storage capacity (19.6 wt%), non-toxicity and high stability under ambient conditions.1 Hydrogen stored in the AB complex can be released by either thermolysis2 or solvolysis.3 Since high temperature is required for the former,4 the latter reaction is highly advantageous for hydrogen generation from AB. However, hydrogen stored in AB can be released at an appreciable rate via hydrolysis only in the presence of a suitable catalyst (eqn (1)).5,6 Therefore, the development of efficient and stable catalysts under moderate conditions is vital for practical applications.| |
 | (1) |
A number of catalysts have been tested in hydrogen generation from the hydrolysis of AB, including transition metal nanoparticles such as platinum, rhodium, ruthenium, palladium, cobalt and nickel.7,8 Although rhodium, platinum and ruthenium metal nanoparticles have high prices and limited abundance, they are superior to the non-noble metal nanoparticles due to their long life-time and high activity in the hydrolysis of ammonia borane. Therefore the use of noble metal nanoparticles as catalysts has been intensively studied in recent years. Metal nanoparticles exhibit much higher catalytic activity compared to the bulk metal due to the large fraction of atoms on their surface. However, metal nanoparticles tend to aggregate into clumps causing a decrease in catalytic activity.9,10 Titanium dioxide with a large surface area ranging from 10 to 300 m2 g−1 can be used as a support to prevent the aggregation of metal nanoparticles. Titanium dioxide is one of the suitable catalysts for environmental applications because of its non-toxicity, strong oxidizing power and the high stability against corrosion.11 Titanium dioxide has also been extensively studied as a semiconductor material due to its wide band gap and low cost.12
Herein we report the in situ generation, characterization, and catalytic use of rhodium(0) nanoparticles supported on titanium dioxide with particle sizes of about 100 nm, hereafter referred to as Rh(0)@TiO2. Rhodium(III) ions impregnated on the surface of titania particles were reduced by ammonia borane forming the Rh(0)@TiO2 without using any additional reducing agents during the hydrolysis of ammonia borane. The use of in situ generation of Rh(0)@TiO2 provides the opportunity to avoid laborious catalyst preparation steps. Rh(0)@TiO2 was isolated from the reaction solution and characterized using ICP-OES, XRD, TEM, SEM-EDS, XPS and N2 adsorption–desorption techniques. Our report also includes the following major findings: (i) formation of highly dispersed rhodium(0) nanoparticles on the surface of titanium dioxide with particle sizes in the range 1.3–3.8 nm. (ii) Remarkable catalytic activity of Rh(0)@TiO2 in hydrogen generation from the hydrolysis of AB with a turnover frequency of 260 min−1 at 25 ± 0.1 °C. (iii) Reusability of Rh(0)@TiO2 providing the complete hydrolysis of AB generating 3 mole H2 per mole of AB even in the fifth use of the catalyst.
Experimental section
Materials
Rhodium(III) chloride trihydrate (RhCl3·3H2O), titanium(IV) oxide (anatase), and ammonia-borane (AB, 97%) were purchased from Aldrich. Deionized water was distilled by a water purification system (Milli-Q System). All glassware and Teflon-coated magnetic stir bars were cleaned with acetone, followed by copious rinsing with distilled water before drying in an oven at 150 °C.
Characterization
The rhodium content of the Rh(0)@TiO2 sample was determined by Inductively Coupled Plasma Optical Emission Spectroscopy (ICP-OES, Leeman-Direct Reading Echelle) after the sample was completely dissolved in a mixture of HNO3–HCl (1
:
3 ratio). Transmission electron microscopy (TEM) was performed on a JEM-2100F (JEOL) microscope operating at 200 kV. A small amount of powder sample was placed on the holey carbon grid of the transmission electron microscope. Samples were examined at magnification between 100 and 400 K. Scanning electron microscope (SEM) images were taken using a JEOL JSM-5310LV at 15 kV and 33 Pa in a high-vacuum mode without metal coating on the carbon support. The X-ray photoelectron spectroscopy (XPS) analysis was performed on a Physical Electronics 5800 spectrometer equipped with a hemispherical analyzer and using monochromatic Al Kα radiation of 1486.6 eV, the X-ray tube working at 15 kV, 350 W and pass energy of 23.5 keV. 11B NMR spectra were recorded on a Bruker Avance DPX 400 with an operating frequency of 128.15 MHz for 11B.
Preparation of rhodium(III) ions impregnated on TiO2
TiO2 (1000 mg) was added to a solution of RhCl3·3H2O (53.97 mg) in 100 mL H2O in a beaker. This slurry was stirred at room temperature for 72 h and then the Rh3+@TiO2 sample was isolated by centrifugation and washed with 100 mL of distilled water and the remnant was dried at 120 °C for 12 h in the oven.
In situ formation of rhodium(0) nanoparticles supported on TiO2 and concomitant catalytic hydrolysis of AB
Rhodium(0) nanoparticles supported on TiO2 (Rh(0)@TiO2) were in situ generated from the reduction of Rh3+@TiO2 during the catalytic hydrolysis of AB. Before starting the catalyst formation and concomitant catalytic hydrolysis of AB, a jacketed reaction flask (20 mL) containing a Teflon-coated stir bar was placed on a magnetic stirrer (Heidolph MR-301) and thermostated to 25.0 ± 0.1 °C by circulating water through its jacket from a constant temperature bath. Then, a graduated glass tube (60 cm in height and 3.0 cm in diameter) filled with water was connected to the reaction flask to measure the volume of the hydrogen gas to be evolved from the reaction. Next, 20 mg powder of Rh3+@TiO2 (0.24 wt% Rh) was dispersed in 10 mL distilled water in the reaction flask thermostated at 25.0 ± 0.1 °C. Then, 31.8 mg AB (1.0 mmol H3N·BH3) was added into the flask and the reaction medium was stirred at 1000 rpm. After adding ammonia borane, rhodium(0) nanoparticles were formed and the catalytic hydrolysis of AB started immediately. The volume of hydrogen gas evolved was measured by recording the displacement of the water level every 30 s at a constant atmospheric pressure of 693 Torr. The reaction was stopped when no more hydrogen evolution was observed. In each experiment, the resulting solutions were filtered and the filtrates were analyzed by 11B NMR and conversion of AB to the metaborate anion was confirmed by comparing the intensity of signals in the 11B NMR spectra of the filtrates.
Determination of activation energy for hydrolysis of AB catalyzed by Rh(0)@TiO2
In a typical experiment, the hydrolysis reaction was performed starting with 10 mL of 100 mM (31.8 mg) AB solution and 20 mg Rh3+@TiO2 (0.24 wt% rhodium, [Rh] = 0.046 mM) at various temperatures (25, 30, 35, 40, 45 °C) in order to obtain the activation energy.
Reusability of Rh(0)@TiO2 in hydrolysis of AB
After the complete hydrolysis of AB started with 10 mL of 100 mM AB (31.8 mg H3NBH3), and 100 mg Rh3+@TiO2 (0.24 wt% rhodium, [Rh] = 0.233 mM) at 25 ± 0.1 °C, the catalyst was isolated as a powder by centrifugation and dried at 120 °C in an oven after washing with 20 mL of water. The isolated samples of Rh(0)@TiO2 were weighed and redispersed in 10 mL solution of 100 mM AB for a subsequent run of hydrolysis at 25 ± 0.1 °C.
Determination of the catalytic lifetime of Rh(0)@TiO2 in the hydrolysis of AB
The catalytic lifetime of Rh(0)@TiO2 in the hydrolysis of AB was determined by measuring the total turnover number (TTO). Such a lifetime experiment was started with a 50 mL solution containing 0.046 mM Rh(0)@TiO2 and 30 mM AB at 25.0 ± 0.1 °C. When all the ammonia-borane present in the solution was completely hydrolyzed, more AB was added and the reaction was continued in this way until no hydrogen gas evolution was observed.
Results and discussion
Rhodium(0) nanoparticles supported on titanium dioxide were in situ generated from the reduction of Rh3+@TiO2 during the catalytic hydrolysis of AB. First, rhodium(III) ions were impregnated on titania with particle sizes of 100 nm from an aqueous solution of rhodium(III) chloride yielding Rh3+@TiO2 and then reduced by AB at room temperature. Both reduction of rhodium(III) to rhodium(0) and hydrogen release from the hydrolysis of AB occur concomitantly when the AB solution is added to a suspension of Rh3+@TiO2. The progress of the hydrolysis of AB was followed by monitoring the change in hydrogen pressure which was then converted into the equivalent H2 per mole of AB, using the known 3
:
1 H2
:
AB stoichiometry (eqn (1)).
Characterization of rhodium(0) nanoparticles supported on TiO2
Rhodium(0) nanoparticles supported on titania (Rh(0)@TiO2), in situ formed during the hydrolysis of AB, could be isolated from the reaction solution as a powder by centrifugation and characterized by ICP-OES, XRD, SEM-EDS, TEM, XPS and N2 adsorption–desorption techniques. Rhodium content of Rh(0)@TiO2 was determined by ICP-OES and found as 0.24 wt% Rh loading on the titania surface. The N2 adsorption–desorption analysis gave the surface area of titania as 10.71 m2 g−1. Since the rhodium content of Rh(0)@TiO2 was very low, it is difficult to understand the existence of rhodium(0) nanoparticles on the surface of titania by N2 adsorption–desorption analysis. Comparison of the XRD patterns of TiO2, Rh3+@TiO2 and Rh(0)@TiO2 with a rhodium loading of 0.24 wt% Rh, given in Fig. 1a–c, respectively, clearly shows that there is no change in the characteristic diffraction peaks of TiO2 (PDF card 21-1272). This observation indicates that the host material remains intact after impregnation and reduction of rhodium(III) ions; there is no noticeable alteration in the framework lattice or change in the crystallinity. There is no observable peak attributable to rhodium nanoparticles in Fig. 1b and c, probably because of the low rhodium loading on the TiO2.
 |
| | Fig. 1 Powder XRD patterns of (a) TiO2, (b) Rh3+@TiO2, (c) Rh(0)@ TiO2 with a 0.24 wt% Rh loading. | |
The SEM image of Rh(0)@TiO2 with a rhodium loading of 0.24 wt% in Fig. 2a shows the presence of nearly monodispersed titania nanoparticles of 100 nm size. The SEM-EDS spectrum of Rh(0)@TiO2 with a rhodium loading of 0.24 wt% in Fig. 2b indicates the presence of the framework elements of TiO2 (Ti, O). Due to the low rhodium loading on TiO2, the presence of rhodium nanoparticles could not be observed in the SEM analysis.
 |
| | Fig. 2 (a) SEM image and (b) SEM-EDS spectrum of Rh(0)@TiO2 with a 0.24 wt% Rh loading. | |
Fig. 3 shows the TEM images of Rh(0)@TiO2 with a rhodium loading of 0.24 wt% taken with different magnifications, which indicate that (i) highly dispersed rhodium(0) nanoparticles are formed on the surface of TiO2 with particle sizes in the range 1.3–3.8 nm (mean diameter: 2.8 ± 0.7 nm) and (ii) the impregnation of rhodium(III) followed by reduction to rhodium(0) causes no change in the framework lattice of titania in agreement with the XRD results.
 |
| | Fig. 3 TEM image of Rh(0)@TiO2 with a rhodium loading of 0.24 wt% at (a) 100 nm, (b) 50 nm, (c) 20 nm, (d) 10 nm, (e) histogram of Rh(0)@TiO2 showing particle size distribution. | |
The composition of Rh(0)@TiO2 formed in situ during the hydrolysis of AB and the oxidation state of rhodium were also studied by XPS. The survey-scan XPS spectrum of Rh(0)@TiO2 with a rhodium loading of 0.24 wt%. (Fig. 4) shows that rhodium is the only element detected in addition to the TiO2 framework elements (Ti, O). High resolution Rh 3d XPS of a Rh(0)@TiO2 sample given in the inset of Fig. 4 shows two prominent bands at 305.8 eV and 311.4 eV which can readily be assigned to rhodium(0) 3d5/2 and 3d3/2, respectively.13,14 The bands at 309.7 eV and 313.8 eV (colored green in the inset of Fig. 4), might be attributed to rhodium oxides, which might be formed during the XPS sampling.14
 |
| | Fig. 4 X-ray photoelectron (XPS) spectrum of Rh(0)@TiO2 sample with a rhodium loading of 0.24 wt% Rh. The inset gives the high resolution scan and deconvolution of Rh 3d bands. | |
Catalytic activity of Rh(0)@TiO2 in hydrolysis of AB
Before starting with the investigation of the catalytic activity of Rh(0)@TiO2 in the hydrolysis of AB, a control experiment was performed to check whether titanium dioxide shows any catalytic activity in the hydrolysis of AB at the same temperature used in this study. In a control experiment starting with 1.0 mmol of AB and 20 mg of powdered TiO2 (the same amount as used in catalytic activity tests) in 10 mL of water at 25.0 ± 0.1 °C or 45.0 ± 0.1 °C, no hydrogen evolution was observed over 1 h at both temperatures. This observation indicates that the hydrolysis of AB does not occur in the presence of TiO2 in the temperature range used in this study. However, Rh(0)@TiO2 is found to be a highly active catalyst in the hydrolysis of AB generating 3.0 equivalents of H2 gas per mole of AB in the same temperature range.
Fig. 5a shows the evolution of equivalent hydrogen per mole of AB versus time plot for the hydrolysis of AB (100 mM) using Rh(0)@TiO2 as the catalyst in different rhodium concentrations at 25.0 ± 0.1 °C. The hydrogen generation rate was determined from the linear portion of each plot. For all tests a complete hydrogen release (mol H2/mol H3NBH3 = 3) was observed. Fig. 5b shows the plot of hydrogen generation rate versus initial concentration of rhodium, both in logarithmic scale, which gives a straight line with a slope of 1.12 indicating that hydrolysis of AB is first order with respect to the rhodium concentration. The turnover frequency (TOF), mol of H2 per mol of rhodium per minute, for hydrogen generation from the hydrolysis of AB (100 mM) at 25.0 ± 0.1 °C was determined from the hydrogen generation rate in the linear portion of the plots given in Fig. 5a for experiments starting with 100 mM AB plus Rh(0)@TiO2 with a loading of 0.24 wt% Rh. The TOF value of the Rh(0)@TiO2 catalyst is as high as 260 min−1 (mol H2 per mol Rh min) in hydrolysis of AB at 25.0 ± 0.1 °C. TOF values of the reported catalysts used in the hydrolysis of AB are listed in Table 1 for comparison. As clearly seen from the comparison of values listed in Table 1, Rh(0)@TiO2 provides a remarkable TOF value in the hydrolysis of AB as compared to the other ruthenium, rhodium and palladium catalysts.
 |
| | Fig. 5 (a) mol H2 per mol H3N·BH3 versus time graph for various rhodium concentrations in Rh(0)@TiO2 for the hydrolysis of AB (100 mM) at 25.0 ± 0.1 °C; (b) the logarithmic plot of hydrogen generation rate versus the concentration of Rh; ln(rate) = 1.12 ln[Rh] + 4.34. | |
Table 1 Catalytic activity of various reported catalysts used in the hydrolysis of AB
| Entry |
Catalyst |
TOF (min−1) |
Ea (kJ mol−1) |
TTO |
Ref. |
| 1 |
Ru@MWCNT |
329 |
33 |
26 400 |
15 |
| 2 |
Rh(0)@TiO2 |
260 |
65.5 |
37 350 |
This study |
| 3 |
Laurate-stabilized Rh(0) |
200 |
43.6 |
80 000 |
16 |
| 4 |
Ru(0)PSSA-co-MA |
172 |
54 |
51 720 |
17 |
| 5 |
Ru(0)@hap |
137 |
58 |
87 000 |
18 |
| 6 |
Ni@Ru |
114 |
44 |
— |
19 |
| 7 |
Ru/carbon |
113 |
76 |
— |
20 |
| 8 |
Ru/graphene |
100 |
11.7 |
— |
21 |
| 9 |
ZFS Rh(0) |
92 |
66.9 |
47 200 |
22 |
| 10 |
RuNPs@ZK-4 |
90.2 |
28 |
36 700 |
23 |
| 11 |
Ru(0)NP/laurate |
75 |
47 |
5900 |
24 |
| 12 |
Pd@Co/graphene |
37.5 |
— |
— |
25 |
| 13 |
Co35Pd65/C annealed |
35.7 |
— |
— |
26 |
| 14 |
2.1 wt% RGO@Pd |
26.3 |
40 |
— |
27 |
| 15 |
Rh/γ-Al2O3 |
— |
21 |
— |
28 |
The catalytic hydrolysis of AB was carried out at various temperatures in the range of 25–45 °C starting with Rh(0)@TiO2 (loading = 0.24 wt% Rh and [Rh] = 0.116 mM) plus 100 mM AB in 10 mL of water. The rate constants for the hydrogen generation at different temperatures were calculated from the slope of the linear part of each plot given in Fig. 6a and used for the calculation of activation energy (Ea = 65 ± 2 kJ mol−1) from the Arrhenius plot in Fig. 6b. The activation energy for hydrolysis of AB catalyzed by Rh(0)@TiO2 is comparable to the literature values reported for the same reaction using other catalysts (see Table 1).
 |
| | Fig. 6 (a) The evolution of equivalent hydrogen per mole of AB versus time plot for the hydrolysis of AB starting with Rh(0)@TiO2 (0.116 mM Rh) and 100 mM AB at various temperatures. (b) The Arrhenius plot for the Rh(0)@TiO2 catalyzed hydrolysis of AB. ln k = −7883.5(T−1) + 27.27. | |
Reusability of the Rh(0)@TiO2 catalyst was tested in successive experiments performed using the catalyst isolated from the reaction solution after a previous run of hydrolysis of AB. After the completion of hydrogen generation from the hydrolysis of AB starting with 0.233 mM Rh3+@TiO2 plus 100 mM AB in 10 mL aqueous solution at 25.0 ± 0.1 °C, the catalyst was isolated by centrifugation and washed with 10 mL of water. After washing, the isolated sample of Rh(0)@TiO2 was redispersed in 10 mL solution containing 100 mM AB and a second run of hydrolysis was started immediately and continued until the completion of hydrogen evolution. The hydrogen generation process was repeated five times. After the fifth use in the hydrolysis of AB, Rh(0)@TiO2 preserved only 7.0% of the initial catalytic activity. The reusability tests reveal that Rh(0)@TiO2 is still active in the subsequent runs of hydrolysis of AB providing a release of 3.0 equivalent H2 per mole of NH3BH3 (Fig. 7).
 |
| | Fig. 7 Percentage of initial catalytic activity of Rh(0)@TiO2 ([Rh] = 0.233 mM) in successive runs after reuse for the hydrolysis of ammonia borane (100 mM). | |
The catalytic activity of the filtrate solution obtained by centrifugation of the solid materials after the first run of the hydrolysis was also tested in the hydrolysis of AB (100 mM) under the same conditions. As shown in Fig. 8, the filtrate solution shows no catalytic activity in the hydrolysis of AB. This observation supports the conclusion that there is no leaching of rhodium into the solution during the hydrolysis and suggests that the rhodium(0) nanoparticles supported on TiO2 are kinetically competent and a heterogeneous catalyst in the hydrolysis of ammonia borane.
 |
| | Fig. 8 The evolution of equivalent hydrogen per mole of AB versus time plot for the hydrolysis of AB (100 mM) starting with Rh(0)@TiO2 (0.233 mM Rh) (black △), and the filtrate solution obtained by centrifugation of the solid materials after the first run, (red △), at room temperature. | |
The catalytic lifetime of Rh(0)@TiO2 was determined by measuring the total turnover number (TTO) in the hydrolysis of ammonia borane. A catalyst lifetime experiment was performed starting with 20 mg Rh3+@TiO2 (rhodium loading = 0.24 wt% Rh, and [Rh] = 0.0466 mM) in 100 mL solution of AB at 25.0 ± 0.1 °C. Fig. 9 shows the variation in turnover number (TON) and turnover frequency (TOF) in the course of reaction. The TOF value decreases expectedly as the rhodium(0) nanoparticles catalysts are deactivated during the lifetime experiment because of the increasing concentration of metaborate ion. Rhodium(0) nanoparticles supported on TiO2 provide 37
350 turnovers over 20 h in the hydrolysis of AB at 25.0 ± 0.1 °C before deactivation. As shown in Table 1, the TTO value of Rh(0)@TiO2 for the hydrolysis of ammonia borane is comparable to the literature values reported for the same reaction using other catalysts.
 |
| | Fig. 9 The variation in turnover number (TON) and turnover frequency (TOF) during the catalytic lifetime experiment performed starting with 20 mg Rh(0)@TiO2 (rhodium loading = 0.24 wt% Rh, and [Rh] = 0.0466 mM) in 100 mL solution of AB at 25.0 ± 0.1 °C. | |
Conclusions
In summary, rhodium(0) nanoparticles supported on titania were reproducibly prepared from the reduction of Rh3+@TiO2 during the catalytic hydrolysis of ammonia borane. Rhodium(III) ions were impregnated on titanium dioxide from the aqueous solution of rhodium(III) chloride and then reduced by ammonia borane at room temperature. Highly dispersed rhodium(0) nanoparticles with particle sizes in the range 1.3–3.8 nm on titanium dioxide were prepared and characterized by a combination of advanced analytical techniques. Rh(0)@TiO2 shows high catalytic activity in hydrogen generation from the hydrolysis of ammonia borane providing a turnover frequency value up to 260 min−1 at 25.0 ± 0.1 °C. Rh(0)@TiO2 is a long-lived catalyst providing 37
350 turnovers in hydrogen generation from the hydrolysis of ammonia borane at 25.0 ± 0.1 °C. Rh(0)@TiO2 is a reusable catalyst as it provides the complete hydrolysis of ammonia borane generating 3 mole H2 per mole of AB even in the fifth use. The results of quantitative kinetic studies on the hydrogen generation from the hydrolysis of ammonia borane show that the hydrolysis reaction is first order in rhodium concentration and the activation energy is 65.5 ± 2 kJ mol−1 for the hydrogen generation catalyzed by Rh(0)@TiO2. High catalytic activity and simple preparation procedures make Rh(0)@TiO2 a very attractive catalyst for the hydrolysis of ammonia borane.
Acknowledgements
Partial support by Turkish Academy of Sciences is gratefully acknowledged. We would like to thank Emrah Yıldırım, Seçkin Öztürk and İlker Yıldız for ICP-OES, TEM and XPS analyses, respectively.
Notes and references
- T. Umegaki, J.-M. Yan, X.-B. Zhang, H. Shioyama, N. Kuriyama and Q. Xu, Int. J. Hydrogen Energy, 2009, 34, 2303–2311 CrossRef CAS PubMed.
- M. Ramzan, F. Silvearv, A. Blomqvist, R. H. Scheicher, S. Lebeque and R. Ahuja, Phys. Rev. B: Condens. Matter Mater. Phys., 2009, 79, 132102–132104 CrossRef.
- Q. Xu and M. Chandra, J. Power Sources, 2006, 163, 364–370 CrossRef CAS PubMed.
- G. Wolf, J. Baumann, J. Baitalow and F. P. Hoffmann, Thermochim. Acta, 2000, 343, 19–25 CrossRef CAS.
- M. Yadav and Q. Xu, Energy Environ. Sci., 2012, 5, 9698–9725 CAS.
- M. Zahmakıran and S. Özkar, Nanoscale, 2011, 3, 3462–3481 RSC.
- S. Özkar, in Batteries, Hydrogen Storage and Fuel Cells, ed. S. L. Suib, Elsevier, Amsterdam, 2013, pp. 165–189 Search PubMed.
- Z. H. Lu and Q. Xu, Funct. Mater. Lett., 2012, 5, 1230001–1230009 CrossRef.
- S. Özkar and R. G. Finke, J. Am. Chem. Soc., 2002, 124, 5796–5810 CrossRef PubMed.
- S. Özkar and R. G. Finke, Langmuir, 2002, 18, 7653–7662 CrossRef.
- O. K. Varghese, M. T. J. LaTempa and C. A. Grimes, Nano Lett., 2009, 9, 731–737 CrossRef CAS PubMed.
- X. Chen and S. S. Mao, Chem. Rev., 2007, 107, 2891–2959 CrossRef CAS PubMed.
- Y. Baer, P. F. Heden, J. Hedman, M. Klasson, C. Nordling and K. Siegbahn, Phys. Scr., 1970, 1, 55–65 CrossRef CAS.
- V. Mevellec, A. Nowicki, A. Roucoux, C. Dujardin, P. Granger, E. Payen and K. Philippot, New J. Chem., 2006, 30, 1214–1219 RSC.
- S. Akbayrak and S. Özkar, ACS Appl. Mater. Interfaces, 2012, 4, 6302–6310 CAS.
- F. Durap, M. Zahmakıran and S. Özkar, Appl. Catal., A, 2009, 369, 53–59 CrossRef CAS PubMed.
- Ö. Metin, S. Sahin and S. Özkar, Int. J. Hydrogen Energy, 2009, 34, 6304–6313 CrossRef PubMed.
- S. Akbayrak, P. Erdek and S. Özkar, Appl. Catal., B, 2013, 142–143, 187–195 CrossRef CAS PubMed.
- G. Z. Chen, S. Desinan, R. Nechache, R. Rose, F. Rose and D. L. Ma, Chem. Commun., 2011, 47, 6308–6310 RSC.
- S. Basu, A. Brockman, P. Gagare, Y. Zheng, P. V. Ramachandran, W. N. Delgass and J. P. Gore, J. Power Sources, 2009, 188, 238–243 CrossRef CAS PubMed.
- N. Cao, W. Luo and G. Cheng, Int. J. Hydrogen Energy, 2013, 38, 11964–11972 CrossRef CAS PubMed.
- M. Zahmakıran and S. Özkar, Appl. Catal., B, 2009, 89, 104–110 CrossRef PubMed.
- M. Zahmakıran, Mater. Sci. Eng., B, 2012, 177, 606–613 CrossRef PubMed.
- F. Durap, M. Zahmakıran and S. Özkar, Int. J. Hydrogen Energy, 2009, 34, 7223–7230 CrossRef CAS PubMed.
- J. Wang, Y.-L. Qin, X. Liu and X.-B. Zhang, J. Mater. Chem., 2012, 22, 12468–12470 RSC.
- D. Sun, V. Mazumder, Ö. Metin and S. Sun, ACS Nano, 2011, 5, 6458–6464 CrossRef CAS PubMed.
- B. Kılıç, S. Şencanlı and Ö. Metin, J. Mol. Catal. A: Chem., 2012, 361–362, 104–110 CrossRef PubMed.
- M. Chandra and Q. Xu, J. Power Sources, 2007, 168, 135–142 CrossRef CAS PubMed.
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