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Journal of Nanomaterials
Volume 2015, Article ID 175605, 5 pages
http://dx.doi.org/10.1155/2015/175605
Research Article

Growth of BiFeO3 Microcylinders under a Hydrothermal Condition

1School of Science, Lanzhou University of Technology, Lanzhou 730050, China
2State Key Laboratory of Advanced Processing and Recycling of Non-Ferrous Metals, Lanzhou University of Technology, Lanzhou 730050, China

Received 22 April 2014; Revised 26 September 2014; Accepted 26 September 2014

Academic Editor: Debasis Dhak

Copyright © 2015 L. J. Di 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

BiFeO3 microcylinders were synthesized via a hydrothermal condition. SEM observation reveals that with increasing the hydrothermal reaction time from 6 to 15 h, the microcylinders grow from ~0.7 to ~4.1 μm in height, whereas their diameter remains to be 3.7-3.8 μm with a minor change. The microcylinders are mainly made up of sphere-like grains of 100–150 nm in size. A possible growth mechanism of the BiFeO3 microcylinders is proposed. The photocatalytic activity of the as-prepared BiFeO3 samples was evaluated by the degradation of acid orange 7 under simulated sunlight irradiation, revealing that they possess an appreciable photocatalytic activity. Magnetic hysteresis loop measurement shows that the BiFeO3 microcylinders exhibit a typical antiferromagnetic behavior at room temperature.

1. Introduction

Bismuth ferrite (BiFeO3) with a rhombohedrally distorted perovskite structure has been extensively studied as one of single-phase multiferroic materials in the past few years [1, 2]. BiFeO3 exhibits ferroelectricity with a Curie temperature of ~830°C and antiferromagnetism with a Néel temperature of ~380°C, making it a promising candidate for room-temperature multiferroic applications [3, 4]. Furthermore, BiFeO3 is an important semiconductor with bandgap energy of about 2.2 eV and has a pronounced photocatalytic activity for the degradation of various organic dyes under visible-light irradiation [511]. Generally, the physical and chemical properties of a functional material depend highly on its morphologies, dimensions, sizes, defects, and so forth. To tailor or enhance the properties of the material, it is especially interesting to create nano/microstructures with various morphologies. Up to now, a large number of nano/microstructures of BiFeO3 have been synthesized including microplatelets, microcubes, nanotubes, nanofibers, microflowers, microspheres, microrods, thick film, microoctahedron, and nanoparticles [519]. Various wet chemical methods have been widely used to achieve those nano/microstructures of BiFeO3. Among them, the hydrothermal route has special advantages in tailoring the product morphology. The variation of any parameter in the hydrothermal reaction process, such as reaction temperature and time, mineralizer type and its concentration, pH value, metal ion concentration, and organic additive, could result in morphologically different products. In this work, we report the synthesis of BiFeO3 microcylinders under a hydrothermal route and a possible growth mechanism of the microcylinders is proposed. The photocatalytic activity of as-prepared samples was evaluated by the degradation of acid orange 7 (AO7) under simulated sunlight irradiation.

2. Experimental

0.005 mol of Bi(NO3)3·5H2O and 0.005 mol of Fe(NO3)3·9H2O were dissolved in 20 mL of dilute nitric acid solution. Then to the mixture solution was added 60 mL KOH solution with a concentration of 9 mol·L−1 drop by drop under magnetic stirring, and immediately a dark brown suspension solution was formed. The suspension was ultrasonically treated for 8 min and subsequently stirred vigorously with a magnetic stirrer for 30 min to create a highly uniform mixture. The resulted mixture was sealed in a Teflon-lined stainless steel autoclave of 100 mL capacity and submitted to hydrothermal treatment at 200°C. After different reaction time, the autoclave was cooled naturally to room temperature. The resulting brown precipitate was collected and washed several times with distilled water and absolute ethanol and then dried in a thermostat drying oven at 80°C for 12 h to obtain final BiFeO3 product. By varying the reaction time from 6 to 15 h, several BiFeO3 samples were prepared.

The phase purity of the samples was examined by means of  X-ray powder diffraction (XRD) with Cu Kα radiation. The morphology of the samples was observed by field-emission scanning electron microscope (SEM). The ultraviolet- (UV-) visible diffuse reflectance spectra were measured using a UV-visible spectrophotometer with an integrating sphere attachment. A vibrating sample magnetometer (VSM) was used to measure the magnetic hysteresis loops of the samples at room temperature.

The photocatalytic activity of the products was evaluated by degrading AO7 in aqueous solution under simulated sunlight irradiation from a 200 W xenon lamp. The initial AO7 concentration was 5 mg·L−1 and the BiFeO3 loading was 0.1 g in 200 mL of AO7 solution. Before illumination, the mixed solution was ultrasonically treated for 15 min in the dark to make BiFeO3 particles uniformly dispersed. During the photocatalysis process, the water-jacketed reactor was cooled with water-cooling system to keep the solution at room temperature. After irradiation for 8 h, the reaction solution was centrifuged for 10 min at 3000 r·min−1 to remove BiFeO3 particles. The AO7 concentration was determined by measuring the absorbance of the solution at a fixed wavelength of 484 nm using an UV-visible spectrophotometer. The percentage degradation is defined as , where and are the AO7 concentrations before and after irradiation, respectively.

3. Results and Discussion

Figure 1 shows the XRD patterns of BiFeO3 samples prepared at the reaction time of 6, 9, and 15 h (the corresponding samples are termed S-6, S-9, and S-15, resp.). For these samples, all the diffraction peaks can be indexed in terms of the rhombohedral structure of BiFeO3 with space group (PDF card number 74-2016). No traces of other phases are detected in the XRD patterns, revealing high purity of the as-prepared products. The widths of the diffraction peaks undergo no obvious change between the samples, indicating that they have nearly the same grain or subgrain size.

Figure 1: XRD patterns of BiFeO3 samples prepared at the reaction time of 6, 9, and 15 h (the corresponding samples are termed S-6, S-9, and S-15, resp.).

Figure 2 shows the SEM images of the as-prepared BiFeO3 samples, revealing the synthesis of cylinder-like microparticles. When the hydrothermal reaction time is 6 h, the resulting sample consists of microcylinders with an average diameter of ~3.7 μm and height of ~0.7 μm (Figure 2(a)). When the reaction time is increased to 9 h, the obtained microcylinders have a diameter of ~3.8 μm and height of ~1.7 μm (Figure 2(b)). Further prolonging of the reaction time up to 15 h leads to the formation of microcylinders with a diameter of ~3.8 μm and height of ~4.1 μm (Figure 2(c)). This implies the continuous growth of BiFeO3 microcylinders along the direction of height with increasing the reaction time, whereas their diameter undergoes minor change. Figure 2(d) shows an enlarged view of the SEM image of Figure 2(b), revealing that the microcylinders are mainly made up of sphere-like grains of 100–150 nm in size.

Figure 2: SEM images of BiFeO3 samples. (a) S-6, (b) S-9, (c) S-15, and (d) enlarged image of sample S-9.

Figure 3 shows a possible growth mechanism of the cylinder-like BiFeO3 particles. Initially, Bi3+ and Fe3+ ions react with OH ions to produce amorphous Bi(OH)3 and Fe(OH)3 precipitates, and then the hydroxides undergo an attack of the mineralizer, KOH, to dissolve and form ion groups. These species undergo nucleation and growth when critical supersaturation is reached, leading to the formation of BiFeO3 nanocrystals. The nascent nanocrystals come together or self-assemble to form cylinder-like aggregates. This self-organization process can be understood according to the oriented-attachment growth mechanism, where the driving force is the reduction of overall surface energy [20, 21]. At the initial stage of the self-organization, thin or disk-like microcylinders with a diameter of about 3.7-3.8 μm are constructed from BiFeO3 nanocrystals. With increasing the reaction time, BiFeO3 nanocrystals are continuously attracted to attach on the surface of the microcylinders, leading to their continuous growth along the height direction, whereas their diameter undergoes minor change.

Figure 3: Schematic illustration of the growth mechanism for cylinder-like BiFeO3 particles.

Figure 4(a) shows the UV-visible diffuse reflectance spectra of BiFeO3 samples and Figure 4(b) gives the corresponding first derivative of the reflectance with respect to wavelength (i.e., ). It is seen that the samples have a similar absorption edge at ~568 nm, which is assigned to the electron transition from valence band to conduction band according to the theoretical results [22]. From the absorption edge, the bandgap energy of the samples is obtained to be 2.18 eV.

Figure 4: (a) UV-visible diffuse reflectance spectra of BiFeO3 samples and (b) the corresponding first derivative of the diffuse reflectance spectra.

Figure 5 shows the photocatalytic degradation of AO7 over BiFeO3 samples as a function of irradiation time , along with the blank experimental result. AO7 appears to be stable under simulated sunlight irradiation in the absence of photocatalyst, and its degradation percentage is less than 7% after 8 h of exposure. When BiFeO3 samples are used as the photocatalyst, the degradation of AO7 is obviously enhanced, indicating an appreciable photocatalytic activity of the samples. The degradation percentage of AO7 after 8 h irradiation with samples S-6, S-9, and S-15 is about 56%, 28%, and 19%, respectively. The sample S-6 exhibits the highest photocatalytic activity, which is mainly ascribed to its relatively small particle size. Generally small particle size and large surface area to volume ratio is required to achieve good photocatalytic activity since the photocatalytic reaction occurs dominantly on the catalyst surface [23].

Figure 5: Photocatalytic degradation of AO7 over BiFeO3 samples as a function of irradiation time along with the blank experiment result.

Figure 6 shows the magnetic hysteresis loops of BiFeO3 samples measured at room temperature, revealing a nearly linear dependence of the magnetization on applied magnetic field. This indicates that all the samples exhibit an antiferromagnetic behavior at room temperature. It is well known that BiFeO3 has a helical antiferromagnetic spin structure with a period of ~62 nm [24]. This helimagnetic structure will be destroyed in nanosized BiFeO3, making the spin compensation incomplete. As a result, weak ferromagnetism is generally observed for nanosized BiFeO3 and exhibits an increasing trend with reducing the grain size [10, 25]. However, BiFeO3 samples synthesized in this work crystallize in relatively large-sized microcrystals, which inhibits the observation of macroscopic magnetization.

Figure 6: Magnetic hysteresis loops of BiFeO3 samples measured at room temperature.

4. Conclusions

Cylinder-like BiFeO3 particles were successfully prepared by a hydrothermal method. It is found that the height of the resulted BiFeO3 microcylinders has a dependence on the hydrothermal reaction time. With prolonging the reaction time from 6 to 15 h, the height of the microcylinders increases from ~0.7 to ~4.1 μm, whereas their diameter undergoes a minor change (3.7-3.8 μm). The microcylinders are constructed from sphere-like BiFeO3 nanocrystals of 100–150 nm in size. Photocatalytic experimental results demonstrate that the BiFeO3 microcylinders exhibit an appreciable photocatalytic activity toward the degradation of AO7 under simulated sunlight irradiation. Magnetic hysteresis loop measurement reveals an antiferromagnetic behavior in the BiFeO3 microcylinders at room temperature.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Acknowledgments

This work was supported by the National Natural Science Foundation of China (Grant nos. 51262018 and 11264023) and the Hongliu Outstanding Talents Foundation of Lanzhou University of Technology (Grant no. J201205).

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