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Open Access Nano Express

Morphology-Controllable Synthesis of CeO2on a Pt Electrode

Y Fu12, ZD Wei123*, MB Ji3, L Li3, PK Shen4* and J Zhang3

Author affiliations

1 State Key Laboratory of Power Transmission Equipment & System Security and New Technology, Chongqing University, Chongqing, 400044, China

2 School of Chemistry and Chemical Engineering, Chongqing University, Chongqing, 400044, China

3 School of Material Science and Engineering, Chongqing University, Chongqing, 400044, China

4 The State Key Laboratory of Optoelectronic Materials and Technologies, Sun Yat-Sen University, Guangzhou, 510275, China

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Citation and License

Nanoscale Research Letters 2008, 3:431-434  doi:10.1007/s11671-008-9177-6

The electronic version of this article is the complete one and can be found online at:


Received:13 August 2008
Accepted:11 September 2008
Published:30 September 2008

© 2008 to the authors

Abstract

Nanoscale cerium dioxides with shape of nanoparticles, nanorods, and nanotubes were electrochemically synthesized. The morphology of CeO2was modulated by changing electrode potential and potential direction. CeO2nanorods and CeO2nanotubes were synthesized via the potentiostatic and cyclic voltammeteric methods, respectively. The morphology and structure of the obtained CeO2were characterized by field emission scanning electron microscope (FESEM) and X-ray diffraction (XRD). A possible formation mechanism has been suggested to illuminate the relationship between the preparation condition and the morphology of CeO2.

Keywords:
CeO2; Nanorod; Nanotube; Electrosynthesis

Introduction

The one-dimension (1D) nanostructure has attracted much attention since the discovery of carbon nanotubes (CNTs) in 1952 [1] and has offered great potential for applications in the electric devices, sensors, and others uses [2]. Controlled synthesis of inorganic nanoparticles now is one of the important topics in colloid and material chemistry for their shape-dependent properties and potentials of self-assembly as building blocks-artificial atoms with diverse superstructures and mesocrystals [3,4]. Much effort has been devoted to the design and preparation of nanostructures with different shapes and sizes. The morphology-controllable synthesis of nanostructured metal compounds, such as PbSe [5], ZnO [6,7], In(OH)3[8], SnO2[9], and V2O5[10], has been successfully developed.

As one of the most active rare earth materials, ceria (cerium oxide, CeO2) has been extensively used in catalysts, fuel cells, solar cells, and polishing materials [11,12]. Stimulated by promising applications and the fantastic properties, much attention has been directed to the controlled synthesis of CeO2 nanostructured materials. Up to now, several strategies have been demonstrated to fabricate CeO2 nanotubes, such as arc discharge, chemical vapor deposition, template-directed synthesis, and hydrothermal treatment. CeO2 nanostructured materials with ordered mesoporous cerium oxides [13], (100) oriented CeO2 films [14], nanorods [15], nanowires [16], nanotubes [17-19], nanocubes [20], nanospheres [21], and nanobelts [22] have been reported. Most recently, Han et al. [18] reported the production of ceria nanotubes via a two-step procedure, precipitation at 100 °C and aging at 0 °C for 45 days. Tang et al. [19] also reported layer-structured rolling Ce(OH)3 nanotubes through an alkali thermal-treatment process under oxygen-free conditions. Evidently, the methods used for synthesis of CeO2 nanostructured materials are usually complicated and time-consuming. An effective method is necessary for production of high-quality ceria nanotubes in terms of yield, uniformity, and shape control. However, it has been a challenge for the effective synthesis of CeO2 nanostructured materials so far.

In this work, we report for the first time one-step synthesis of CeO2nanoparticles, nanorods, and nanotubes via an electrochemically synthesized route. The morphology was modulated by changing the electric field, strength, and direction. A possible formation mechanism of CeO2nanostructured materials has been suggested to illuminate the relationship between the preparation condition and the morphology of yielded CeO2.

Experimental

Preparation of CeO2Nanostructured Materials

CeO2was potentiostatically and cyclic voltammeterically synthesized on a Pt electrode, and accordingly, the synthesized CeO2are named as ps-CeO2and cv-CeO2, respectively. In the potentiostatically synthesized CeO2, the Pt electrode potential was kept at 1.2 V (versus KOH saturated Hg/HgO) for a length of 30, 85, and 130 s in a bath of 0.05 M Ce(NO3)3 · 6H2O and 0.1 M NH4NO3at room temperature. The pH of the solution was adjusted to 6 by NH4OH. In the cyclic voltammeterically synthesized cerium oxide, CeO2was prepared on a Pt electrode by cycling potential between 0.5 and 1.4 V at a sweep rate of 20, 30, and 50 mV s−1, respectively, for 120 min in the same bath as used in the potentiostatical synthesis.

Morphologies Characterization

XRD analysis of CeO2was carried out on the D/max-1200 diffractometer (Japan) using a Cu KαX-ray source operating at 45 kV and 100 mA, scanning at the rate of 4°/min with an angular resolution of 0.05° of the 2θscan to get the XRD patterns. The morphologies of the CeO2were studied on a FEI Nova 400 field emission scanning electron microscope (FESEM) (Peabody, Netherland).

Results and Discussion

Morphologies of Synthesized CeO2Nanostructured Materials

Figure 1 shows the XRD pattern of the synthesized ps-CeO2 sample. The diffraction peaks corresponding to the different planes of CeO2 are marked in Fig. 1. The diffraction peaks can be indexed to the face-centered cubic structure of CeO2 (space group Fm3 m) with a lattice constant of 0.5410 nm according to JCPDS 78-0694 [15,23].

thumbnailFigure 1. XRD spectrum of ps-CeO2prepared at 1.2 V for 30 s

Figure 2 shows the growth history of ps-CeO2 generated potentiostatically at 1.2 V with different lengths of anodic oxidation. As seen, only a few of nanoparticles with size of 15–50 nm (measured from the SEM micrograph and consistent with the crystallite size calculated from XRD) are present on the smooth Pt surface as the anodic oxidation lasts for 30 s. When the anodic oxidation lasts for 85 s, more CeO2 spherical crystallites form. Meanwhile, a clear grain boundary is also observed. It indicates that obtained CeO2 crystallites are constituted by the oriented aggregation of small CeO2 nanoparticles. The diameter of the CeO2 nanoparticles is in the range of 20–100 nm calculated by statistical software with the FESEM. With the time of anodic oxidation further increasing to 130 s, number of isolated nanoparticles began to reduce, but nanorods are nearly the sole products as illustrated in Fig. 2c, in which CeO2 nanorods plus many tiny interconnected nanoparticles are present. The similar structure CeO2 was synthesized previously via ultrasonication approach with aid of polyethylene glycol as a structure-directing agent [15]. Figure 3 shows morphologies of CeO2 nanotubes synthesized by the way of CV between 0.5 and 1.4 V at different sweep rates. Figure 3 shows the curve degree of CeO2 nanotubes increases with the potential sweep rate. That is, the curve degree of CeO2 nanotubes increases with the potential sweep rates from 20, and then 30, and finally to 50 mV s−1, which is really interesting. Nanoscale CeO2 synthesized potentiostatically has rod-shape morphology, but those synthesized cyclic-voltammeterically has curve-shape morphology. In short, the morphologies of CeO2 sized in nanoscale from nanoparticles, nanorods, and to nanowires can be fabricated by simply changing the potential direction and time of anodic oxidation. Why does the curve degree of CeO2 nanotubes increase with potential sweep rates? The following abecedarian mechanism about CeO2 nanotube growth was suggested.

thumbnailFigure 2. FESEM images of ps-CeO2prepared at 1.2 V for 30 s (a), 85 s (b), and 130 s (c)

thumbnailFigure 3. FESEM images of cv-CeO2prepared at a sweep rate of 20 mV s−1(a), 30 mV s−1(b), and 50 mV s−1(c) for 2 h

Possible Formation Mechanism of CeO2Nanotubes

Oxidation of Ce (III) to CeO2can be accomplished electrochemically in reaction (1) or chemically in reaction (2). In this work, CeO2is synthesized electrochemically.

(1)

(2)

Since an instantaneous nucleation and growth mechanism cannot explain the morphology-controllable synthesis of CeO2, the formation of CeO2nanorods and nanotubes is assumed to experience the process as illustrated in Fig. 4. The CeO2nanoparticles adsorb OHions and fuse them together by hydrogen bonding. Adsorbed OHon the surfaces of CeO2will further adsorb Ce3+ions, and then OHand Ce3+ions combine to CeO2with one electron release. OHand Ce3+ions are electrically adsorbed on the surfaces of CeO2in an oriented manner under pulling force of the direct current electric field and fused together. It leads to the formation of CeO2nanorods. Thus, if OHand Ce3+ions are electrically adsorbed on the surfaces of CeO2under pulling force of a continuously changed electric field direction and fused together, it will certainly lead to the formation of CeO2curved nanotubes. The stronger the electric field direction changes, the more frequently the position of adsorbed OHand Ce3+ions on the surfaces of CeO2moves, the more curved the CeO2nanotubes will be. It is not strange why CeO2nanotubes with a different curved degree were generated at different potential sweep rates.

thumbnailFigure 4. Possible mechanism of CeO2nanorod and nanotubes growth

Conclusions

CeO2nanoparticles, nanorods, and nanotubes were electrochemically fabricated via a one-step route. The morphology of CeO2can be modulated by changing electrode potential and potential direction. At constant electric field, such as the way of potentiostatic, OHand Ce3+ions are electrically adsorbed onto the surfaces of CeO2in an oriented manner under pulling force of the direct current electric field and fused together. It leads to the formation of CeO2nanorods. Curved CeO2nanotubes can be produced by a continuously changing electric field direction, such as cyclic voltammetry. The curved degrees of CeO2nanotubes can be modulated by changing electrode potential sweep rates.

Acknowledgments

This work was financially supported by NSFC of China (Grant Nos 20476109 and 20676156), by the Chinese Ministry of Education (Grant No. 307021), China National 863 Program (2007AA05Z124), Chongqing and Guangdong Sci. & Tech. Key Projects, China (CSTC2007AB6012, 2007A010700001, and 2007B090400032).

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