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Pengzhen Cui1 , Jiali Wang1 , Zumin Wang1 , Jun Chen1 , Xianran Xing1 , Lianzhou Wang2 , and Ranbo Yu1,2 ()
Department of Physical Chemistry, University of Science and Technology Beijing, Beijing 100083, China
Nanomaterials Centre, School of Chemical Engineering and AIBN, The University of Queensland, St. Lucia, Brisbane, QLD 4072, Australia
ABSTRACT
Hollow microspheres of two bismuth oxychlorides, BiOCl and Bi24O31Cl10, were successfully synthesized using carbonaceous microsphere sacrificial templates. The phase evolution from BiOCl to Bi24O31Cl10 was easily realized by heating the former at 600 ° C. With a uniform diameter of about 200 nm, an average shell thickness of 40 nm, and basic nanosheets of <20 nm, the hollow microspheres of both BiOCl and Bi24O31Cl10 showed high visible light photocatalytic activity towards the degradation of Rhodamine B (RhB). Besides the effective photosensitization process and efficient photointroduced carrier separation, the high photocatalytic activity was believed to result from their hollow-structuredependent large visible light absorption. Moreover, as a chlorine-deficient analogue, the Bi24O31Cl10 hollow spheres possessed a narrower band gap, more dispersive band structure, and higher photocarrier conversion efficiency, which further helped them to exhibit better photocatalytic activity.
1 Introduction
In recent years, the study of semiconductor photocatalysis has gained much interest because of its potential application to environmental pollution purification [1, 2] and energy conversion [3–5]. As bismuth is a p-block metal with a d10 configuration, bismuth-based materials, such as Bi2O3 [6], Bi2WO6 [7], and BiVO4 [8], have shown efficient photocatalytic activity in wastewater purification. Furthermore, they are better materials owing to their low toxicity and natural abundance. Bismuth oxychlorides are of immense importance because of their outstanding optical and electrical properties. They have also shown promise in catalysis applications [9, 10]. Although BiOCl is a wide band gap semiconductor (~3.2 eV), when constructed as a nanostructure, it can exhibit photocatalytic activity upon the degradation of organic dyes under visible light irradiation by either increasing the surface-to-volume ratio or exposing a specific crystal plane. Zhang’s group found that the {001} and {010} facet-dominant BiOCl single-crystalline nanosheets can be synthesized at a pH of 1 and 6, respectively, via a hydrothermal route [11]. Upon dehalogenation, BiOCl can be converted to Bi24O31Cl10. As a p-block semiconductor, Bi24O31Cl10 is an ideal candidate to become a photocatalyst and photoanode in dye sensitized solar cells [12]. Consequently, further enhancement of its photocatalytic properties is of great significance. Doping and defect are the most widely used methods to improve the photocatalytic activity of semiconductors [13, 14].
The specific performance of materials is influenced not only by their composition and crystal phase, but also by their microscale structure and morphology [15–19]. In an effort to improve its unique material properties, a variety of BiOCl microstructures, including 1D nanofibers and fibers [20, 21], 2D nanosheets and nanoplates [22–24], and 3D nanowire arrays, nanoflowers, and hierarchical architectures [25–29], have been synthesized by different synthetic procedures such as electro-spinning, sol-gel, and hydrolyticsolvothermal synthesis. These efforts revealed that the nanostructure design of BiOCl could be used to improve its photocatalytic activity [10, 29]. However, corresponding research regarding Bi24O31Cl10 is scarce because it is generally formed from the dehalogenation of BiOCl, which destroys the original nanostructure of BiOCl and results in the loss of any property improvements.
Recently, hollow micro-/nano-structure materials have attracted tremendous attention because of their large surface-to-volume ratio and short transport length of mass or charge. They have been recognized as promising materials in lithium ion batteries [30, 31], gas sensitization [32], and photocatalysis [33–35]. Building hollow structures from bismuth-based materials may renew their application in the area of photocatalysis. Among all synthetic methods, sacrificial templating utilizing carbonaceous microspheres is of the greatest interest because of its high controllability of physical properties, such as size, shape, and structure, of samples [36]. As a straightforward and facile method, the sacrificial template method uses functional groups on reactive surfaces, which facilitate the coating of cationic metal ions and nanoparticles [31, 32]. Thus far, hollow spheres of various single-metal oxides, such as TiO2, Co3O4, and Fe2O3, and partial binary-metal oxides, such as ZnFeO4 [37], have been synthesized by templating methods. However, to our knowledge, there are no reports about hollow microspheres formed from bismuth-based materials. The large size of Bi3+ makes it difficult to be absorbed on the surface and transported in a template; consequently, insufficient adsorption hinders the formation of hollow compact structures after removing the template.
In this work, we developed a facile procedure to produce hollow microspheres of bismuth oxychloride composed of nanocrystal subunits using carbonaceous microspheres as sacrificial hard templates. By varying synthetic parameters, BiOCl and Bi24O31Cl10 hollow spheres were obtained. Both BiOCl and Bi24O31Cl10 hollow spheres exhibited high photocatalytic activity towards the degradation of Rhodamine B (RhB). Moreover, the formation and catalytic mechanisms are discussed here in detail.
2 Experimental
2.1 Material and preparation
All chemicals used in the present experiments were obtained from commercial sources as analytical reagents and used as received without further treatment. In a typical synthesis of carbonaceous spheres, sucrose (130 g) was dissolved in deionized water (250 mL) to form a clear solution. The solution was then added into a 500 mL Teflon-lined autoclave. The autoclave was then heated at 200 ° C for 2 h. Subsequently, when the autoclave was cooled to room temperature, the precipitates were collected and washed with deionized water and 100% ethanol. They were then dried at 80 ° C for 6 h.
A typical synthesis process for the bismuth oxychloride hollow spheres is as follows: 1.46 g of Bi(NO3)3·5H2O was dissolved in 30 mL of hydrochloric acid solution (1 mol·L−1 ), followed by the addition of 0.6 g carbonaceous spheres to form a black suspension. The suspension was magnetically stirred for 6–8 h at room temperature to ensure Bi3+ absorption by carbonaceous spheres. Lastly, the suspension was collected and watered alternately with deionized water and ethanol to obtain precursors. It was then air-dried at 80 ° C. BiOCl hollow spheres (BiOCl-HS) and Bi24O31Cl10 hollow spheres (Bi24O31Cl10-HS) were obtained by calcination of the precursors under ambient conditions at 400 and 600 ° C, respectively. For comparison, the BiOCl bulk was synthesized by a precipitation method, and Bi24O31Cl10 bulk was synthesized by calcination of the BiOCl bulk under ambient conditions at 600 ° C.
2.2 Characterization
The crystal structures of the samples were characterized X-ray diffraction (XRD, X’ pert PRO, PANalytical) with Cu-Kα radiation. To determine the composition and calcination temperatures of the obtained precursors, thermogravimetric (TG) curve and differential scanning calorimetry (DSC) data of the precursors were recorded on a thermal analysis instrument (DTG-60AH). The morphologies and microstructures of the as-prepared samples were observed using a scanning electron microscope (FE-SEM, ZEISS SUPRATM 55) and transmission electron microscopy (TEM, JEM-2100, accelerating voltage 200 kV). The UV–vis diffffuse reflectance spectra were obtained on a TU-1901 spectrophotometer in the 230–850 nm wavelength range. Brunauer–Emmett–Teller (BET) surface areas of the samples were analyzed by nitrogen adsorption–desorption measurement on a Quantachrome Autosorb-1MP sorption analyzer with prior degassing under vacuum at 200 ° C. A 300 W Xe lamp (CEL-HXF300) was used as a light source with a cutoff filter and employed for the visible-light irradiation (λ > 420 nm).