Abstract
Solar energy transformation over semiconductor-based photocatalysis is an ideal solution to environmental problems and future sustainability. Layered bismuth oxyhalides (BiOX, X = Cl, Br or I) are very attractive and promising photocatalysts in the environment fields. This review summarizes recent advances on the design of BiOX to enhance energy converting efficiency. Especially, the emerging techniques to enhance the photocatalytic behaviors of BiOX are discussed, including non-metal/metal doping, heterojunction engineering, carbon interfacing, coupling with noble metals, defect engineering, and morphology tuning. The application of BiOX composites in wastewater remediation is also reviewed in terms of organic photocatalytic oxidation and heavy metal ion photocatalytic reduction. Finally, the future chances and challenges of BiOX photocatalysts for practical application are summarized. In all, this review well underlies the innovative preparation of BiOX products for environment-related purposes.
Introduction
Water pollution and unavailability of clean and inexpensive water are among the biggest challenges of the 21st century (
Qu et al., 2013). Water shortage attacks 1/3 of the global population, and clean drinking water is inaccessible to one billion people (
WHO/UNICEF Joint Monitoring Programme for Water Supply and Sanitation and UNICEF, 2005). The remarkable enhancement in living standards since the industrial revolution increases both the demand for freshwater and the amount/variety of polluting chemicals in water (
Tollefson, 2011;
Richardson, 2012;
Carlsen et al., 2013). The existence of emerging contaminants, including toxic heavy metal ions, antibiotics, and endocrine disrupting chemicals (
Fatta-Kassinos et al., 2011;
Bueno et al., 2012), in water resources made the EU Commission Services establish a new guidance on environmental quality criteria to guarantee the quality of drinking water and to preserve the aquatic environment. Among the existent technologies for water and wastewater treatment, the most common methods include adsorption, membranes, chemical oxidation, and biological treatments. However, these technologies are relatively inefficient in eliminating emerging and persistent organic compounds. The advanced oxidation processes (AOPs) based on
in situformation of largely reactive species (HO• and O
2-•) can convert organic contaminants into less harmful substances (e.g., CO
2and H
2O) (
Lee and Park, 2013). Various AOPs such as photochemical oxidation (UV/O
3and UV/H
2O
2), chemical oxidation (O
3and Fenton reagents), and heterogeneous photocatalysis (UV/TiO
2) (
Hidalgo et al., 2007;
Malato et al., 2007) are available for wastewater processing. Among the most explored and economical AOPs, photocatalysis needs only light energy without extra chemicals and runs at mild pressure and temperature (
Lin et al., 2015;
Landge et al., 2021). Semiconductor materials are by far the most common form of photocatalysts since they can be photoexcited by photons of energy equal to or above the bandgap energy to produce charge carriers for surface redox reactions. The overall process of photocatalysis takes five steps (
Herrmann, 1999;
Herrmann, 2005):
1) mass migration of reactants from the bulk medium to the catalyst–fluid interfacial region;
2) surface adsorption of the reactants;
3) photocatalyst activation and surface reaction:
a absorption of photons by the catalyst
b generation of electron-hole (e−-h+) pairs
c diffusion of photogenerated charges to the surface and
d surface transfer of the photocharges to the reactants (i.e., surface reaction)
4) product desorption from the photocatalyst surface; and
5) mass migration of the products from the interface to the bulk fluid.
In particular, for a semiconductor photocatalyst, when irradiated light arrives at its valance band (VB), a VB electron is excited to the conduction band (CB), forming electron-hole pairs. Most of the photocharges that fail to transport away very quickly will recombine. The photocharges can also be trapped by various bulk and surface sites during the diffusion to the surface. As a result, only a fraction of the photocharges will arrive at the surface to catalyze redox reactions (Hoffmann et al., 1995). Figure 1 displays all the reactions on the catalyst surface mentioned above.
FIGURE 1
Common photocatalysts (e.g., ZnO and TiO2) (Raizada et al., 2016) mostly can degrade organic pollutants in water under UV irradiation (<5% solar spectrum), but their applications are limited by the low light-gathering ability, fast photocharge carrier recombination, and narrow feasible range of pH. Therefore, photocatalysts driven by visible light (∼43% of solar light) with wide pH tolerance and fast division of photocharge carriers are needed. Recently, bismuth-based photocatalysts such as Bi2O3 (Gadhi et al., 2016; Jalalah et al., 2015; Oudghiri-Hassani et al., 2015), Bi2WO6 (Fu et al., 2005; Zhang and Zhu, 2005; Zhang et al., 2009), BiVO4 (Yu and Kudo, 2006; Luo et al., 2011), Bi2MoO6 (Bi et al., 2007; Zhang et al., 2010), BiPO4 (Pan and Zhu, 2011; Pan and Zhu, 2010), Bi2Ti2O7 (Yao et al., 2004), (BiO)2CO3 (Ni et al., 2016), BiOCOOH (Xiong et al., 2011a), and bismuth oxyhalides (BiOX, X = Cl, Br, I) (Henle et al., 2007; Huang and Zhu, 2008; Huizhong et al., 2008; Zhang et al., 2008; Chang et al., 2010; Chen et al., 2013; Cheng et al., 2014; Ye et al., 2014; Yang et al., 2018) have been used in visible-light–driven water purification. Especially, BiOX with its chemical inertness, photocorrosion tolerance, and harmlessness in aqueous media has received wide attention. The BiOX becomes crystals in matlockite (PbFCl-type) tetragons (space group P4/nmm). The crystal lattice comprises [Bi2O2]2+ slice interlayers between halogen anion dual-slabs, gathering along the z-axis by the nonbonding (van der Waals) interaction (Figure 2A) (Chen et al., 2013). This two-dimensional layered structure of BiOX facilitates the formation of an inner electric field between halogen and [Bi2O2]2+ slabs owing to the transformation of photoexcited electron-hole pairs (Zhang et al., 2006). The VB of BiOX is constituted by X p (X = Cl, Br or I) orbitals and O 2p orbitals (Tu et al., 2012; Zhang et al., 2012; Zhao et al., 2013) while the CB comprises Bi 6p orbitals (Cao J. et al., 2012; Zhang et al., 2013). Density functional theory (DFT) calculation indicates the distance between two slabs is elongated with the rise of the halogen atom count, following the narrowed bandgap, such as BiOCl (∼3.2 eV) (Ma Z. et al., 2017), BiOBr (∼2.6 eV) (Li K. L. et al., 2014; Kong et al., 2016), and BiOI (∼1.8 eV) (Xiao and Zhang, 2010; Ye et al., 2011) (Figure 2B). Thereby, the light absorbing range can be prolonged from ultraviolet to visible light.
FIGURE 2
In 2006, Zhang et al. prepared the BiOCl using the hydrolysis method, and for the first time, they found that BiOCl had a better performance than TiO2 (P25, Degussa) on photocatalytic degradation of methyl orange (MO) dye (Zhang et al., 2006). In addition, Zhang and co-workers synthesized hierarchical BiOCl nanoplate microspheres using the one-pot solvothermal method. The as-obtained BiOCl showed 1.7 times higher photocatalytic activity than TiO2 toward MO degradation (Zhang et al., 2008). In 2015, Ding et al. prepared the BiOCl hierarchical microsphere (2–50 nm) through controlling pH in the reaction precursor, and the samples showed a preferable photocatalytic activity for rhodamine B (RhB) dye degradation (Ding et al., 2015). Although BiOCl has better performance than TiO2, the large band gap energy (∼3.2 eV) limited their application under visible light.
BiOBr had a narrower band gap (∼2.6 eV) than BiOCl and thus has been used under visible irradiation in recent years. Zhang et al. prepared the BiOBr microspheres using the ethylene glycol (EG) assisting solvothermal method (Zhang et al., 2008). Due to the narrow band gap of BiOBr, it shows 2.5 times and 3.5 times higher catalytic activity than TiO2 under UV and visible light irradiation. In addition, the flower-like hierarchical architectures of BiOBr was prepared by Jia et al., who employed tetrabutylammonium halide as halogen sources in ethanol solvent (Jia et al., 2015). The as-obtained BiOBr can degrade rhodamine B and salicylic acid under visible light.
The BiOI owned the narrowest band gap energy (∼1.8 eV) in BiOX and thus had the best performance under visible light in principle. However, the significant recombination of photocharges in pristine BiOI limited their photocatalytic activity. The BiOI hierarchical nanospheres show a better adsorption (57.4% removal) on MO dye than photocatalytic activity (∼42.6% removal) (Li R. et al., 2015). Therefore, the BiOI was always used as light harvesting for extending the light adsorption of composites. For example, Zhang et al. prepared the TiO2/BiOI p-n junction by using the hydrothermal-solvothermal route. The light absorption of composites can be extended to the visible region, and the separation efficiency of photocharges in TiO2 can be improved. As a result, the TiO2/BiOI composites show 16.6 times higher methylene blue degradation than TiO2 (Zhang Y. et al., 2021).
Although the favorable bandgap can be obtained by changing halogen atoms, the photocatalytic ability of pristine BiOX is still inefficient due to the fast electron-hole recombination and the decreased redox ability (Guo et al., 2021). In other words, BiOX can hardly keep responsive light sensitivity, rapid carrier movement, and high redox capability at the same time.
Many methods can be used to restrict charge carrier recombination in BiOX during heterogeneous photocatalysis. One common way is to decorate BiOX materials with another semiconductor to form type II heterojunctions, such as Bi2WO6 (Meng and Zhang, 2015; Xiang et al., 2016; Wang F. et al., 2018; Wang J. et al., 2019; Tahmasebi et al., 2019), TiO2 (Park et al., 2012; Yang J. et al., 2014; Choi et al., 2016; Yao et al., 2020), and Cu2O (Cao et al., 2015; Zhang Y. et al., 2020a). Another strategy is the deposition of noble metals: the generally lower Fermi energy of metal nanoparticles than that of BiOX promotes electron migration from the semiconductor to the metal via Schottky contact. The most common decorative metals include platinum (Pt), silver (Ag), and gold (Au) owing to their noble and/or catalytic properties (Yu et al., 2013; Gao et al., 2014; Bi et al., 2016; Liu et al., 2018; Zhou S. et al., 2019; Yadav et al., 2021). They all function as electron sinks/reservoirs, spatially isolating the electrons from the VC photoholes of BiOX, and as more-active sites and co-catalysts for photocatalytic reduction. Another useful method for extracting photoelectrons from BiOX to prevent charge carrier recombination is to prepare composites with carbon materials, particularly graphene-based nanomaterials (Chou et al., 2016; Dai and Zhao, 2017; Lee et al., 2017; Garg et al., 2018a; Su et al., 2018; Sharma N. et al., 2019; Zhang W. et al., 2019; Zhu et al., 2019; Yadav et al., 2020; Alansi et al., 2021; Sharma et al., 2022). Because of the fast electron motion in graphene, photoelectrons from the CB of BiOX to graphene are easily isolated from the BiOX surface. The other methods including defect engineering, Bi-rich strategy, morphology, and thickness control have also been reported and summarized in various review studies (Di et al., 2017; Li et al., 2018; Xiong et al., 2020). However, few studies focus on the intuitive comparison of photocatalytic activity of BiOX prepared by different methods for wastewater treatment.
Herein, we summarize recent advances in BiOX photocatalysts for wastewater remediation. First, we briefly probe into the preparation schemes for BiOX, which is regarded as essential from the application perspective. Then, various strategies to improve BiOX photocatalytic activity are discussed, such as facet management, element doping, heterojunction, defect engineering, and Schottky barriers. After that, the behaviors, decomposition routes of representative organics, and probable mechanisms during degradation by bismuth catalysts are assessed. Last, the problems of BiOX-based photocatalytic processes in water environmental use are listed.
Synthetic Methods of BiOX Photocatalysts
Hydro/Solvothermal Method
The hydro/solvothermal method is the most widely used for producing diverse micro/nanostructured BiOX. Specifically, a chemical reaction proceeds in a sealed pressure vessel at high temperature and pressure in water or an organic solvent. The products often possess high crystallinity without calcination. Huo et al. prepared BiOBr nanosheets by hydrothermally treating Bi(NO3)3∙5H2O and KBr at 160°C for 12 h (Li K. L. et al., 2014). A similar procedure was extended to the preparation of BiOCl (Xiong et al., 2011b) and BiOI (Li H. et al., 2013). Different from the hydrothermal route which uses a precursor water solution, the solvothermal route adopts various solvents (e.g., methanol (Vadivel et al., 2014), ethylene glycol (Liu et al., 2014), and glycerol (Liu Z. et al., 2012)) to synthesize the precursor solution. This route allows the increment of pressure and temperature relative to the hydrothermal route (Liu Z. et al., 2012). Zhang et al. first produced 3D BiOX microspheres by using the solvothermal route with ethylene glycol (Figure 3) (Zhang et al., 2008) Furthermore, difference in solvents during this route impacts the growing direction of BiOX crystals. Xiong et al. studied the effect of alcohol chain length on the thermal preparation of BiOBr by using methanol, n-butanol, and n-hexanol as solvents at 180°C for 5 h in a stainless steel vessel (Xiong et al., 2016). When the carbon chain length of n-alcohol was prolonged, the characteristic diffraction peaks of BiOBr at the (102) and (110) facets were sharper and stronger, indicating the improvement of BiOBr crystallization.
FIGURE 3
The adoption of precursors during preparation directly affects the BiOX facets. As reported, BiOBr with exposed (001) facet is photocatalytically more active, because the (001) facet has much lower surface energy than other facets and BiOBr materials have an intraelectric field along the [001] direction (Zhao et al., 2012). The use of ionic liquid Br instead of KBr led to the generation of BiOBr with exposed (001) facet, because the ionic liquid is passivating and can lower the facet surface energy (Mao et al., 2014).
The addition of surfactants such as polyvinylpyrrolidone (PVP) and hexadecyl-trimethyl-ammonium bromide can reportedly regulate morphology. Liu et al. made BiOBr flower-nanospheres with 32.9 m2/g surface area via the solvothermal procedure using Bi(NO3)3⋅5H2O, PVP (M = 45,000∼58,000), bromide [C16min]Br, and ethylene glycol as precursors while keeping the reaction at 140°C for 24 h (Liu and Wu, 2017). Hao et al. compared the effect of PVP on BiOI photocatalytic activity (Hao et al., 2012). With PVP, the BiOI nanosheets self-aggregated to form 3D hierarchical microspheres, which exhibited a higher photocatalytic activity in tetracycline hydrochloride (TCHC) degradation than 2D-BiOI nanoplates (removal rate 94 vs. 44%).
Alcoholysis/Hydrolysis
Both hydrolysis and alcoholysis methods offer mild conditions for synthesis of BiOX, but the products have nonuniform dimensions. For instance, BiOCl nanostructures were synthesized from 6 h of BiCl3 hydrolysis at 65°C using acetylacetone as an assisting solvent under acidic conditions (Armelao et al., 2012). Song et al. prepared 21- to 85-nm-thick BiOCl nanosheets from hydrolysis of Bi(NO3)3 with HCl and Na2CO3 by keeping it at ∼ pH2 for 30 min at ambient temperature (Song et al., 2017). Zhang et al. compared the photocatalytic activity of BiOBr prepared by hydrolysis and alcoholysis and added 0.5 g of BiBr3 to 15 ml of solvent of water or isopropyl alcohol at room temperature (Li R. et al., 2015). Then the suspension was heated at 20, 40, or 60°C for 10 min, and the pH was kept at 9. The BiOBr from hydrolysis was nanosheet-shaped and composed of the best crystallinity and unique (102) facets, while the BiOBr from alcoholysis was flower-like with exposed (110) facets. Both showed a superior photocatalytic activity toward methyl orange (MO) degradation, but the BiOBr from hydrolysis had higher photostability after 4 cycles. Huang et al. prepared BiOBr with different shapes (0D spherical quantum dots, 1D nanorods, 2D nanosheets, and 3D hierarchical architectures) through room-temperature hydrolysis (Figure 4) (Han et al., 2020) Different bismuth or bromine sources, solvents, capping agents, or surfactants affected the morphology of BiOBr during hydrolysis. The direct hydrolysis of BiI3 was used to prepare BiOI by Su et al., who used the as-obtained BiOI to degrade Rhodamine B under simulated solar light (Su et al., 2014).
FIGURE 4
Template Method
This method alters the morphology of BiOX mainly by modulating the crystal nucleation and growth during the synthesis. Nanomaterial synthesis by the template method basically takes three steps (Xie et al., 2016). 1) A template is produced. 2) The target product is synthesized under the action of the template via precipitation, sol-gel, hydrothermal, or other common synthetic method. 3) The template is removed. Cui et al. adopted carbonaceous microspheres as a template to adsorb Bi3+ and Cl−, followed by sintering up to 400°C to form hollow BiOCl microspheres, which were in a shell thickness of 40 nm and a diameter of 200 nm (Cui et al., 2016). With a butterfly wing as a biological template, Yan et al. prepared hierarchical BiOCl (Yan et al., 2019). BiOI was also used as a self-sacrifice template to construct Bi4O5I2/Bi5O7I and BiOI/Bi4O5I2 heterojunctions from simple calcination (Cheng et al., 2020). The BiOBr self-sacrifice template was also used for the formation of BiOBr/Bi4O5Br2 (Li P. et al., 2020).
Other Methods
Microwave, co-precipitation, and calcination can also be used to synthesize BiOX. For example, Chen et al. prepared BiOBr with a 3D flower-like structure after 27 min of microwave processing (Li et al., 2012). The BiOBr showed a Brunauer, Emmett and Teller (BET) surface area of 63.5 m2/g and an outstanding removal ability and fast adsorbing rate over Cr6+ in a wide pH range. Reportedly, the presence of surfactants during microwave processing improved the BiOBr photocatalytic activity (Chen et al., 2017). The BiOCl was also prepared by microwave with the same procedure as BiOBr and showed an excellent visible-light photocatalytic activity for dye Rhodamine B (RhB) (He et al., 2015). Ai et al. prepared the hierarchical porous BiOI using the microwave method. The as-obtained BiOI shows an excellent adsorption ability toward Congo red in water and it can be easily regenerated under light irradiation (Ai et al., 2014).
During preparation of BiOBr by co-precipitation (Lu et al., 2012), Bi(NO3)3 and KBr were mixed in acetic acid water solution, stirred, and aged for 6 h. The BiOCl microflowers were successfully prepared by using a simple co-precipitation method, and it had a better photocatalytic activity under acidic conditions than neutral and alkaline conditions (Wang and Zhang, 2020). The BiOI was also prepared by co-precipitation and EDTA was introduced as the retarder of the reaction and a structure-directing agent in aqueous media. The as-obtained BiOI exhibited a large BET surface area (∼47.5 m2 g−1) and thus had an excellent photocatalytic activity for NO removal (98%) in the gaseous phase (Montoya-Zamora et al., 2017).
The unstable halogen atoms in BiOX can easily escape due to the weak van der Waals forces. Therefore, phase transformation can be achieved by directly heating BiOX. Plate-like Bi24O31Br10 was prepared via sintering of BiOBr at 750°C (Yu C. et al., 2012). A similar process was extended to the synthesis of hollow Bi24O31Cl10 microspheres at 600°C (Cui et al., 2016). The 3D hierarchical bismuth oxyiodides was prepared using the ethylene glycol–assisted in situ hydrolysis method and the subsequent calcination at high temperature. The multiform bismuth oxyiodides obtained at different temperatures exhibit very distinct microstructure and band structure, and their photoabsorption was tuned from 700 to 400 nm in an orderly manner, rendering the adjustable oxidation and reduction ability of band energy levels (Huang et al., 2017).
Various Techniques to Improve Photocatalytic Activity of BiOX
Like any semiconductor-mediated photocatalysis, the maximum efficiency is decided by charge separation/transportation and surface catalytic performance. Inappropriate use of photoelectrons with low thermodynamic energy due to the presence of a positive CB will deteriorate the charge isolation of BiOBr and BiOI. Although BiOCl has a more negative CB, the large bandgap (∼3.22 eV) limits its application under visible light. Therefore, to enhance the visible light and photocatalytic capabilities of BiOX, diverse approaches like heterojunction, metal/nonmetal doping, noble metal deposition, interfacing with carbon materials, defect engineering, etc. can be adopted to strengthen the organic photodegradation efficiency.
Heterojunction
Heterojunction basically refers to the band alignment caused by the interface between two types of semiconductors with unequal band structures. Heterojunction is divided by the band positions of the semiconductors into three types (Yang, 2021). Type II, the most widely used one, offers the best band positions for effective charge carrier isolation, which results in higher photocatalytic activity. The photoelectrons will be transported from the CB of semiconductor A to the CB of semiconductor B for favorable energetics of the relative positions of the CBs (Figure 5A). Holes are transferred at the same time from the VB of semiconductor B to the VB of semiconductor A. Under light illumination, the electrons and holes are spatially isolated from each other, lowering the recombination possibility (Ning et al., 2016). Yang et al. prepared type II Bi2WO6/BiOBr heterojunction via a one-step solvothermal route for degradation of rhodamine B (RhB), methylene blue, and colorless TCHC (Figure 6A) (Ren et al., 2019) Guo et al. prepared BiVO4/BiOCl heterojunction with a higher charge separation rate than pure BiVO4 or BiOCl (Liu et al., 2019). More research on BiOX-based Type II heterojunction can be found in Table 1.
FIGURE 5
FIGURE 6
TABLE 1
| Photocatalysts | Synthesis method | Light source | Improved performances |
|---|---|---|---|
| Heterojunction | |||
| Bi2WO6/BiOBr (Ren et al., 2019) (Type II) | Solvothermal | λ ≥ 420 nm (300 W Xe lamp) | 12 times that of BiOBr and 23 times that of Bi2WO6 for RhB degradation in 60 min |
| S-C3N4/BiOBr (Vinoth and Pandikumar, 2021) (Type II) | Ultrasonic hydrothermal | AM 1.5G, 100 mW/cm2 | 13 times that of BiOBr and 89 times that of S-gC3N4 for PEC water oxidation |
| Bi2SiO5/BiOBr (Chai et al., 2019) (Type II) | Ion exchange | λ ≥ 420 nm (300 W Xe lamp) | 1,253 times that of BiOBr and 25.2 times that of BiVO4 for RhB degradation in 90 min |
| BiVO4/BiOCl (Liu et al., 2019) (Type II) | Ion exchange | AM 1.5G, 100 mW/cm2 | 102 times that of BiOCl and 1.44 times that of BiVO4 for PEC water splitting |
| Bi2S3/BiOCl (Wang Y. et al., 2018) (Type II) | Epitaxial growth | λ ≥ 420 nm, 100 mW/cm2 | 15 times that of BiOCl and 2 times that of Bi2S3 for PEC water splitting |
| CeO2/BiOCl (Wang H. et al., 2020) (Type II) | Precipitation hydrothermal | λ ≥ 420 nm (300 W Xe lamp) | 1.67 times that of BiOCl and 3.37 times that of CeO2 for methyl tetracycline degradation in 120 min |
| g-C3N4/BiOI (Vinoth et al., 2021) (Type II) | Ultrasonic hydrothermal | AM 1.5G, 100 mW/cm2 | 2 times that of BiOI and 11 times that of g-C3N4 for PEC water splitting |
| SnS/BiOI (Juntrapirom et al., 2017) (Type II) | Hydrothermal coprecipitation | λ ≥ 400 nm (50 W Hg lamp) | 1.67 times that of BiOI and 4.97 times that of SnS for MO degradation in 60 min |
| BiOBr/Bi2O2CO3 (Wang J. J. et al., 2020) (p-n junction) | Precipitation conversion | 300 W Xe lamp | 14.7 times that of Bi2O2CO3 and 4.03 times that of BiOBr for RhB degradation in 20 min |
| BiOBr/SnO2 (Wu et al., 2020) (p-n junction) | Hydrothermal | λ ≥ 420 nm (150 W Xe lamp) | 1.5 times that of BiOBr and 12.2 times that of SnO2 for NO removal in 5 min |
| BiPO4/BiOCl (Zhang Z. et al., 2020) (p-n junction) | In situ chemical transformation | 300 W xenon lamp | 3.18 times that of BiOCl for RhB degradation in 90 min |
| BiOI/g-C3N4 (Tian et al., 2020) (p-n junction) | Precipitation | λ ≥ 420 nm (300 W Xe lamp) | 10 times that of g-C3N4 and 4 times that of BiOI for bisphenol A degradation in 4 h |
| TiO2/BiOI (Zhang Y. et al., 2021) (p-n junction) | Hydrothermal | Visible light, 300 mW/cm2 | 16.6 times that of TiO2 and 1.38 times that of BiOI for methylene blue degradation in 60 min |
| BiOI/ZnO (Xiao et al., 2020) (p-n junction) | Hydrothermal | λ ≥ 420 nm (300 W Xe lamp) | 9.2 times that of BiOI and 2 times that of ZnO for methylene blue degradation in 180 min |
| CDs/BiOCl (Lin et al., 2017) (Z-scheme) | Electrochemical | λ ≥ 420 nm (350 W Xe lamp) | 7.62 times that of BiOCl for RhB degradation in 180 min |
| BiOBr/MnFe2O4 (Sin et al., 2020) (Z-scheme) | Hydrothermal | Visible light (105 W compact fluorescent lamp) | 2.85 times that of BiOBr and 6.42 times that of MnFe2O4 for RhB degradation in 80 min |
| BiOBr/BiOIO3 (Jia et al., 2020a) (Z-scheme) | Solvothermal | λ < 400 nm (9 W LED light) | 1.24 times that of BiOIO3 and 4.42 times that of BiOBr for removal of heavy metal mercury in 60 min |
| BiOBr/Bi2MoO6 (Wang S. et al., 2017) (Z-scheme) | Two-step coprecipitation | λ ≥ 420 nm (300 W Xe lamp) | 10.0 times that of pure BiOBr and 54.5 times that of pure Bi2MoO6 for RhB degradation in 25 min |
| AgI/BiOBr (Yu et al., 2018) (Z-scheme) | Solvothermal precipitation | λ ≥ 420 nm (300 W Xe lamp) | 2.75 times that of BiOBr and 52.5 times that of AgI for ciprofloxacin degradation in 60 min |
| SnNb2O6/BiOCl (Jiang et al., 2019) (Z-scheme) | Two-step hydrothermal | λ ≥ 420 nm (250 W Xe lamp) | 10.51 times that of SnNb2O6 and 20.58 times that of BiOCl for benzocaine degradation in 90 min |
| BiOCl/g-C3N4 (Sun et al., 2020) (Z-scheme) | Hydrothermal | Simulated solar light (300 W Xe lamp) | 20.51 times that of BiOCl for tetracycline degradation in 60 min |
| BiOI/Bi2O4 (Qin et al., 2020) (Z-scheme) | Ultrasonic hydrothermal | 100 W LED lamp | 2.81 times that of Bi2O4 and 30 times that of BiOI for RhB degradation in 32 min |
| Co3O4/BiOI (Malefane et al., 2020) (Z-scheme) | Solvothermal | 60 W LED lamp | 80.1 times that of Co3O4 and 13.5 times that of BiOI for ibuprofen degradation in 60 min |
| Elemental doping | |||
| Cu2+-doped BiOBr (Lv et al., 2020) | Solvothermal | λ ≥ 420 nm (300 W Xe lamp) | 2.28 times higher than that of undoped BiOBr for norfloxacin degradation in 90 min |
| Zn2+-doped BiOBr (Zhou J. et al., 2019) | Solvothermal | λ ≥ 420 nm (300 W Xe lamp) | 3.35 times enhancement for the RhB degradation in 30 min |
| Ag/Ti-doped BiOBr (Jiang G. et al., 2012) | Solvothermal reduction | λ ≥ 400 nm (11 W daylight lamp) | 5.11 times enhancement for the RhB degradation in 30 min |
| Sn2+-doped BiOBr (Tu et al., 2015) | Solvothermal | Visible light (500 W Xe lamp) | 2.71 times higher than pure BiOBr for RhB degradation in 16 min |
| Zn2+-doped BiOCl (Li W. T. et al., 2015) | Solvothermal | λ ≥ 420 nm (300 W Xe lamp) | 2.71 times higher than pure BiOCl for the RhB degradation in 60 min |
| Mn3+-doped BiOCl (Pare et al., 2011) | Hydrolysis | Visible light (500 W halogen lamp) | 1.53 times improvement for malachite green photodegradation in 180 min |
| N-doped BiOBr (López-Velázquez et al., 2021) | Microwave-assisted solvothermal | 300–800 nm with an intensity of 30 W/m2 in the UV region | 3.3, 2.2, 4.1, and 1.4 times improvement for bisphenol A, 17β-estradiol, 17α-ethinylestradiol, and 4-tert-octylphenol photodegradation, respectively |
| P-doped BiOI (Ma F.Q. et al., 2017) | Hydrothermal | λ ≥ 420 nm (300 W Xe lamp) | 2.63 times higher than BiOI for RhB degradation in 60 min |
| C-doped BiOBr (Zhang W. et al., 2019) | Hydrothermal | λ ≥ 420 nm (800 W Xe lamp) | 4.7 times enhancement for tetracycline degradation in 25 min |
| S-doped BiOBr (Liu et al., 2021) | Solvothermal | λ ≥ 420 nm (300 W Xe lamp) | 3 times higher than pure BiOBr for ibuprofen degradation in 240 min |
| La3+-doped BiOBr (Yin et al., 2017) | Solvothermal | λ ≥ 400 nm (300 W Xe lamp) | 3.8 and 1.7 times enhancement for RhB in 60 min and ciprofloxacin in 180 min degradation, respectively |
| Y3+-doped BiOCl (Zhong et al., 2020) | Consecutive solvent-based and thermal | Visible light (300 W xenon lamp) | 1.8 times improvement for the tetracycline hydrochloride within 90 min |
| Er ion–doped BiOBr (Xia et al., 2016) | Solvothermal | λ ≥ 400 nm (300 W Xe lamp) | 1.8-fold improvement for ciprofloxacin degradation within 360 min |
| Noble metal deposition | |||
| Ag/BiOBr (Yu et al., 2011) | Photodeposition | Visible light (300-W tungsten lamp) | 14-fold improvement for acid orange II degradation in 40 min |
| Pd/BiOBr (Li X. et al., 2020) | Photodeposition | Xe lamp at 200 mW cm−2 | 1.5 times improvement for photocatalytic selective oxidation of toluene to benzaldehyde |
| Rh, Pd, Pt/BiOCl (Yu et al., 2013) | Photodeposition | 420 nm < λ < 660 nm (150 W tungsten halogen lamp) | 2.1, 2.2, and 3.1 times enhancement for Rh, Pd, and Pt deposited BiOCl for acid orange II degradation |
| Ag/BiOCl (Yu et al., 2017) | Photodeposition | Two 365 nm LED lamps with an average light intensity of 80 mW cm−2 | 2.5-fold improvement for MO degradation |
| Pd/BiOCl (Chen et al., 2014) | Solvothermal | Visible light (300 W Xe lamp) | 2.5-fold enhancement for RhB degradation |
| Au/BiOI (Chang et al., 2021) | Ion sputter | AM 1.5G at 100 mW/cm2 (300 W Xe lamp) | 24-fold improvement in PEC efficiency over bare BiOI |
| Ag/BiOI (Liu H. et al., 2012) | Hydrothermal and photodeposition | λ ≥ 420 nm (500 W Xe lamp) | 4.00, 3.99, and 3.39 times improvement over BiOI in degradation of acid orange II, MO, and RhB, respectively |
| Interfacing with carbon materials | |||
| BiOBr/graphene (Tu et al., 2012) | EG-assisted solvothermal | λ ≥ 420 nm (500 W Xe lamp) | 3 times higher than BiOBr for RhB degradation |
| BiOBr/graphene hydrogel (Chang et al., 2020) | Two-step hydrothermal | Visible light (300 W Xe lamp) | 1.83 times higher than that of BiOBr for degradation of potassium butyl xanthate |
| BiOCl/graphene (Li Z. et al., 2017) | Hydrothermal | Full arc (150 W Xe lamp) | 8.4 and 3.8 times higher than BiOCl for degradation of MO and oxidation of water |
| GO foam/BiOI | In situ deposition | λ ≥ 400 nm (60 W LED spotlight lamp) | 1.84 times improvement for phenol degradation in 150 min |
| BiOI/CNT (Sharma et al., 2021) | Hydrothermal | Visible light (4 × 24 W visible light lamps) | 2 times and 3 times higher than BiOI for degradation of phenol and RhB |
| BiOI-MWCNT (Su et al., 2012) | EG-assisted solvothermal | λ ≥ 400 nm (150 W Xe lamp) | 2.1 times higher than BiOI for degradation of acid orange II in 180 min |
| BiOCl-carbon quantum dots (Di et al., 2015) | Mannitol-assisted solvothermal | λ ≥ 400 nm (300 W Xe lamp) | 2.22 and 2.12 times higher than pure BiOCl for the degradation of RhB in 40 min and degradation of BPA in 120 min |
| Defect engineering | |||
| BiOBr-OV (Li H. et al., 2015) | EG-assisted solvothermal | λ ≥ 420 nm (LED light, 10 W/cm2) | Can generate NH3 under light irradiation versus BiOBr without OV |
| BiOBr-OV (Lyu et al., 2019) | Solvothermal | Full arc (10 W LED lamp) | 3.5 times improvement for tetracycline degradation over BiOBr |
| OV-rich S-doped BiOBr (Wang Q. et al., 2019) | Solvothermal | λ ≥ 420 nm (300 W Xe lamp) | 4.9 and 18.0 times those of pristine BiOBr and OV-poor S-doped BiOBr for 4-CP degradation within 120 min |
| BiOBr-OV (Shi et al., 2018) | Solvothermal | Visible light (300 W Xe lamp) | 3, 2.69, 2, and 1.74 times improvement for degradation of phenol, BPA, RhB, and MO compared with OV-poor BiOBr, respectively |
| BiO1−xCl (Cao et al., 2018) | Diethylene glycol solvothermal | λ ≥ 400 nm (300 W Xe lamp) | Adsorbing 42% ciprofloxacin and 40% doxycycline, no adsorption on BiOCl; degrading ciprofloxacin and doxycycline after 40 min, only 30% removal over BiOCl |
| BiOCl-OV (Song et al., 2021) | Sodium dodecylbenzenesulfonate hydrothermal | λ ≥ 400 nm (Xe lamp) | 1.48 times improvement for the oxytetracycline hydrochloride degradation |
| BiOCl-OV (Cui et al., 2018) | Solvothermal | λ ≥ 420 nm (300 W Xe lamp) | 3.3 times higher for oxygen evolution than OV-poor BiOCl |
| BiOI-OV (Huang et al., 2014) | Solvothermal | λ ≥ 420 nm (500 W Xe lamp) | 1 order-of-magnitude improvement in donor density versus BiOI and 10 times higher photocatalytic activity than BiOI for MO degradation |
| BiOI-OV (Chen et al., 2016) | Glycerol solvothermal | Visible light (300 W Xe lamp) | 3.5 times higher than untreated BiOI nanosheets for MO degradation |
| Facet control | |||
| BiOBr-110 (Peng et al., 2017) | Glucose hydrothermal | λ ≥ 400 nm (300 W Xe lamp) | Degrading 91% MO in 30 min and 100% RhB in 10 min, 60% MO and 70% RhB by BiOBr-001 |
| BiOBr-010 (Wu et al., 2017) | Chemical precipitation | Visible light (300 W Xe lamp) | 3 times improvement of PEC performance over BiOBr-001 |
| BiOBr-010 (Jia et al., 2020b) | pH adjustment | λ < 420 nm (9 W LED lamp) | 1.2 times improvement for Hg oxidation over BiOBr-001 |
| BiOCl-001, BiOCl-010 (Jiang J. et al., 2012) | Hydrothermal | UV or visible light (300 W Xe lamp) | UV: 1.6 times enhancement for MO degradation in BiOCl-001 over BiOCl-010; visible light, 2.5 times higher in BiOCl-010 versus BiOCl-001 |
| Thickness tuning | |||
| Thickness-controllable Bi24O31Br10 nanosheets (Wang C. Y. et al., 2017) | NH4Br hydrothermal | λ ≥ 420 nm (520 W Xe lamp) | Bi24O31Br10 (∼40 nm thickness) is 3.11 and 4.79 times higher than that of Bi24O31Br10 with 80 nm and with 130 nm thickness for tetracycline hydrochloride degradation |
| Morphology control | |||
| BiOI hollow microspheres (Di et al., 2014) | Ionic liquid-assisted microemulsion method | λ ≥ 400 nm (300 W Xe lamp) | BiOI hollow microspheres are 4 times higher than BiOI nanosheets for degradation of RhB in 150 min |
| Bi12O17Br2 nanotubes (Di et al., 2020) | Solvothermal treatment | 300 Xe lamp | Bi12O17Br2 nanotubes, exhibiting 14.4 times higher activity than Bi12O17Br2 nanoplates for CO2 photoreduction |
Summary of BiOX-based composites with improved photocatalytic activity.
Though type-II heterojunction can perfectly isolate electrons-holes in space, the improvement in such isolation across this heterojunction is unable to prevent the ultrafast hole-electron recombination on the semiconductor. Therefore, p-n junction is proposed for greatly effective charge acquisition and isolation. Generally, p- and n-type semiconductors upon contact will constitute a p-n junction with an interfacial space-charge zone due to the electron and hole diffusion and thus generate a built-in electrical potential that can guide the electron and hole migration in the opposite direction (Figure 5B) (Jiang L. et al., 2012; Li L. et al., 2014; Jiang and Li, 2015) When incident light with an energy at least equal to the bandgap values irradiates the p-n junction, both p- and n-type semiconductors can be excited to form electron-hole pairs (Lin et al., 2011; Cao J. et al., 2012; Peng et al., 2014). The electrons are stimulated by the electric field to move to the CB of the n-type semiconductor, and the holes to the VB of the p-type semiconductor. Consequently, the electron-hole pairs are separated in p-n heterojunctions more quickly than in type-II heterojunctions due to the cooperation between the inner electric field and band arrangement (Yu et al., 2010). Wang et al. prepared p-type BiOBr and interfaced with n-type Bi2O2CO3 by precipitation conversion. The photoactivity of BiOBr/Bi2O2CO3 p-n junction is 14.8 folds that of bare Bi2O2CO3 (Wang J. J. et al., 2020). Sun et al. prepared BiOBr/SnO2 p-n heterojunctions to eliminate NO in visible light. Importantly, the charge transfer channels and directions at the BiOBr/SnO2 interface were determined by theoretical calculations (Figure 6B) and experiments (using XPS) (Wu et al., 2020). Similar research was extended to BiOCl and BiOI (Table 1).
Although the above heterojunctions are advantageous in separating photoelectron-hole pairs, the redox ability of these systems is weakened and thus cannot provide sufficient driving force for a specific photocatalytic reaction. Direct Z-scheme heterojunction photocatalysts have been proposed for spatial division of photoelectrons and holes whilst preserving the strong redox ability of two semiconductors (Figure 5C). Under irradiation, the CB photoelectrons of semiconductor A with strong reducing ability and the VB holes of semiconductor B with strong oxidizing ability are preserved. The CB photoelectrons of semiconductor B with low reducing ability and the VB holes of semiconductor A with low oxidizing ability recombine. The 4% CdS/BiOCl heterojunction prepared by Lin et al (Lin et al., 2017) showed a 10% higher photoactivity than pristine BiOCl in elimination of RhB, which was due to the direct Z-scheme mechanism (Figure 6C). In a new Z-scheme BiOBr/MnFe2O4 nanocomposite, spontaneous transfer of photoelectron carriers contributed to the photoelectron-hole division and decelerated the electron-hole recombination (Sin et al., 2020). Other Z-scheme photocatalysts were also reported before (Table 1).
Elemental Doping
Incorporation of transition metal ions into BiOX lattices to generate or modify the electronic states has gained much attention. Furthermore, it may induce lattice defects in BiOX or change crystallinity to prevent electron-hole combination, forming long-lasting carriers. Doping with special metal ions can also enhance light absorption region, which remarkably influences the photoelectrochemical (PEC) performance of semiconductors. Doping with transition metal ions (e.g., Fe3+, Cu2+, and Mn3+) will form impurity energy levels and may induce a redshift in the energy band, which is attributed to the electron transition from impurity bands to the CB or VB. Cu2+ was doped into BiOBr by using the solvothermal method to form the doping level (Figure 7), which strengthened both light absorption and electron-hole isolation efficiency (Lv et al., 2020). Consequently, the Cu2+-doped BiOBr showed a 2.28 times higher visible-light–driven photocatalytic activity relative to pristine BiOBr. A similar method was used to prepare Fe2+-doped BiOBr (Li W. et al., 2017). The doping of tungsten resulted in a bandgap reduction and the generation of an impurity band in the forbidden zone of BiOCl, as confirmed by first-principle theoretical computation and experimental findings. (Yang W. et al., 2014). Other commonly used transitional metal dopants reported in BiOX include Zn2+ (Li J. et al., 2015; Zhou et al., 2019b), Ti4+ (Jiang G. et al., 2012), Al3+ (Weng et al., 2014a), Sn4+ (Tu et al., 2015), and Mn3+ (Pare et al., 2011).
FIGURE 7
The incorporation of non-metal dopants can distribute extra extrinsic electronic levels in the band gap, which greatly affects light adsorption and charge carrier isolation. The main hypothesis is that the VB shifts upward to its maximum level after valence orbitals and local states hybridize from valence orbitals (Chen et al., 2015). Many non-metals such as N, Fen-Qiang Ma et al. (2017), Zhancheng Zhang et al. (2019), Obeid et al. (2020), Liu et al. (2021), and López-Velázquez et al. (2021) were doped into BiOX to improve the photocatalytic activity. Wang et al. prepared the boron-doped BiOBr nanosheets, in which the B dopants form an impurity level to accelerate charge separation (Figure 7G) (Wu et al., 2016) Carbon doping can enhance the internal electric field of Bi3O4Cl and thereby increase bulk-charge separation to 80% (Li et al., 2015). This homogeneous carbon-doped Bi3O4Cl was prepared by using a glucose-hydrothermal method, followed by thermal treatment to allow the diffusion of the carbon dopant in host lattices. A similar method was employed by Jin et al. to prepare C-doped Bi24O31Cl10 from oxytetracycline hydrochloride as a carbon and chlorine source (Jin et al., 2018).
Rare earth metals with a 4f electron shell are rich in electronic energy levels, which function as electron trapping centers for photocharge carriers. Hence, doping with rare earth metals may promote charge separation and overall photocatalytic performance. In the La3+-doped BiOBr microspheres produced by using an ionic liquid ([C16mim] Br)-assisted solvothermal route, (Yin et al., 2017), the substitution of Bi3+ by La3+ was monitored by XRD peak shift, while no La2O3 or another phase of La was found. The La-doped BiOBr significantly increased the photodegradation of ciprofloxacin, which was because La may trap photoelectrons and thus inhibit the electron-hole recombination (Figures 7H–J). Similarly, Y-doped BiOCl improved the visible-light photocatalytic activity in tetracycline decomposition (Zhong et al., 2020). Moreover, europium and erbium were also used as dopants in BiOX recently (Xia et al., 2016).
Noble Metal Modification
Deposition of noble metals (e.g., Ag, Pt, Rh, or Pd) on the surface of BiOX to build a space-charge dividing region (namely, the Schottky barrier) is another effective method to promote photo-charge separation. At the interface between a noble metal and BiOX, the electron transfer from the higher-Fermi-level BiOX to the lower-Fermi-level metal will arrange the Fermi energy levels. The presence of the Schottky barrier endows the metal and the semiconductor with excessive negative and positive charges, respectively. The Schottky barrier also acts as an effective electron trap against electron-hole reconnection in photocatalysis, which often leads to a higher photocatalytic capability. More recently, the deposition of Ag nanoparticles (NPs) on BiOX was found to remarkably improve dye decomposition efficiency under UV or visible light illumination (Yu et al., 2011; Yu C. L. et al., 2012). Li et al. prepared Pd/BiOBr by photodeposition (Figure 8A) and found the existence of Pd initiated the formation of more oxygen vacancies on the surface of BiOBr due to the electron interaction at the Pd–BiOBr interface. The coexistence of Pd and oxygen vacancies on BiOBr facilitates the adsorption of O2 and toluene molecules (Figure 8B). As a result, the Pd/BiOBr interface controls the charge division and activates O2 and toluene, improving the photocatalytic activity of BiOBr by 1.5 times in 99% selective oxidation of toluene to benzaldehyde (Figure 8C) (Li X. et al., 2020) Yu et al. investigated how noble metals (Rh, Pd, and Pt) deposition affected the photocatalytic behaviors of BiOX. The impact of the noble metals ranks as Pt > Pd > Rh under UV and as Rh > Pt > Pd under visible light. The noble metal NPs also function as electron traps to quicken electron-hole division and thus improve the visible light activity (Yu et al., 2013).
FIGURE 8
Interfacing with Carbon Materials
Due to the excellent electrical conductivity, flexibility, and specific surface, carbon materials are ideal supporting scaffolds for homogeneous anchoring of functional nanomaterials. Xu et al. coated hierarchical BiOX (X = Cl or I) on the newly prepared functional carbon nanotubes through ionic layer adsorption and reaction. The nanotubes with outstanding mechanical properties and pollutant absorbing ability were used to tailor the energy gaps of BiOX via covalent bonds (Figure 9A) (Weng et al., 2014b). Similarly, the BiOI/multi-walled carbon nanotube composites prepared by Xiong et al. using the solvothermal method photocatalytically outperformed pure BiOI owing to the interfacial charge-transfer (Figure 9B) (Su et al., 2012). Graphene is another common carbon material to couple with BiOX. Li et al. prepared a BiOBr/graphene composite by an in situ solvothermal route using graphene oxide (Figure 9C). The graphene oxide was reduced to graphene, and BiOBr NPs were formed on the surface. This composite has higher photocatalytic activity in degrading RhB (Tu et al., 2012). Reduced graphene oxide (RGO)/BiOCl hybrids were synthesized by Zhang et al. with graphene oxide as the precursor (Li Z. et al., 2017). The RGO/BiOCl was 8.4 and 3.8 times more photocatalytically active than BiOCl in MO degradation and water oxidation, respectively. This was because the chemical bonding of BiOCl with RGO led to faster charge separation and longer carrier lifetime. It is indicated that chloride vacancies may act as recombination centers to impede photocharge separation (Figure 9D). Carbon quantum dots (CQDs) with quasi-spherical nanoparticles usually <10 nm in diameter have been introduced to BiOX recently. Li et al. prepared the CQD-modified BiOCl which showed the enhanced photocatalytic activity due to superior electron transfer ability of CQDs (Di et al., 2015). Furthermore, the nitrogen-doped CQD–modified BiOBr was prepared by the same group to boost the photodegradation toward ciprofloxacin, rhodamine B, tetracycline hydrochloride, and bisphenol A (Di et al., 2016).
FIGURE 9
Defect Engineering
The creation of defects permits the adjustment of micro/electron structure, atom coordination number, and charge transfer in BiOX. Zhang et al. prepared the [001] facet exposed BiOBr with oxygen vacancy (OV) by using an ethylene glycol–assisted solvothermal method and used it to fix atmospheric N2 to NH3 (Figures 10A,B) (Li et al., 2015d). The sample without OV was also synthesized by further sintering in an O2 atmosphere, and the color turned white (Figure 10C). NH3 was detected over BiOBr with OV, but not in BiOBr without OV (Figure 10D). This was because the OV in BiOBr was the catalytic activation center and can chemisorb N2 on the surface. Similarly, Xue et al. used BiOBr nanosheets with OV to realize N2 to NH3 (Xue et al., 2018). The Bi3O4Br nanosheets with single-unit-cell thickness and confined defects have been controllably prepared by Di et al., who demonstrated that the bismuth vacancy can greatly facilitate the generation of oxygen defects, accounting for the formed oxygen defects in the bismuth oxyhalides (Di et al., 2019). Wang et al. prepared OV-rich S-doped BiOBr by one-step solvothermal treatment. The optimal BB-5S degraded 98% 4-chlorophenol (4-CP) under visible light within 120 min, which was 18.0 and 4.9 times those of OV-poor sulfur-doped BiOBr and pristine ultrathin BiOBr, respectively. Experiments and DFT computation showed a sub-band was formed under the synergy of OVs and S doping, which largely facilitated visible-light absorption capability and inhibited photocharge recombination, thus improving photocatalytic activity (Wang Q. et al., 2019). Cui et al. solvothermally prepared OV-rich BiOCl nanosheets (Cui et al., 2018). A new energy level from OV was verified both theoretically and experimentally. BiOCl nanosheets with OV were capable of photocatalytic oxygen evolution under visible light. Additionally, OV-rich BiOCl displayed a higher visible-light photocurrent and more efficient photocharge division and migration than BiOCl with fewer OVs.
FIGURE 10
Apart from the single vacancies, the effect of surface vacancy pairs in BiOX on photocatalytic activity has been explored recently. When the thickness of BiOX decreased to atomically thin, the atomic-escape energy will be smaller and then surface atoms will escape from the 2D lattice and create vacancies more easily (Di et al., 2018a). Liu and co-workers prepared the Bi24O31Br10 atomic layer with “Bi-O” vacancy pairs by a mild polyvinylpyrrolidone (PVP) self-assembly strategy coupled with pH adjusting (see Figure 10E). In contrast to the perfect surface, Bi24O31Br10 with Bi-O vacancy pairs own large local electric field intensity (Figures 10F,G). Furthermore, the presence of Bi-O vacancy pairs would create an electron delocalization hot spot (Figures 10H,I), where both inflow and outflow of electrons are better favored. Therefore, the separated charges can be effciently delivered to target reactants, significantly enhancing the catalytic reaction rate (Di et al., 2021).
Facet Control
Semiconductor photocatalysts with specific exposed crystal surfaces can improve photo-charge separation and transportation, which further strengthens the photocatalytic performances. In general, surfactants and H+ are used to modulate the exposed crystal surface. Glucose can be the capping and structure-directing agent in preparing one-dimensional rod-like BiOBr with exposed (110) facets (BiOBr-110) (Figure 11A) (Peng et al., 2017). Glucose can interact with the (001) facet of BiOBr NPs to prevent the development of these planes, leading to the generation of ultrathin BiOBr nanosheets with exposed (001) facets. In the meantime, glucose drives the ultrathin nanosheets to gather along the [001] orientation, forming BiOBr nanorods with exposed (110) facets. BiOBr-110 photocatalytically outperforms BiOBr-001 owing to the lower resistance and higher efficiency of charge transfer. Zhao et al. prepared the BiOCl with high ratios of [001] and (Li et al., 2012) facets (BiOCl-H1 and BiOCl-H2, respectively) under various acid conditions (Figure 11D) (Zhao et al., 2020), which remarkably raised the RhB photodegradation efficiency. The apparent rate constant of BiOCl-H2 was 0.0961 min−1, about 2.7 times that of BiOCl-H1 (Figures 11E,F). The Z-scheme facet heterojunction was constructed to accelerate charge separation and transportation (Figure 11D). Zhang et al. found that single-crystal BiOCl nanosheets with exposed [001] facets were more active in direct semiconductor photoexcited MO removal under UV light, but the counterpart with exposed [010] facets was highly active in indirect dye photosensitive decomposition under visible light (Jiang J. et al., 2012).
FIGURE 11
Thickness Tuning
Thickness tuning is another strategy for improving the photocatalytic activity of BiOX. When the thickness of BiOX is reduced, the quantum confinement can be realized to tune the band edge structure, which is favorable for meeting the potential requirement of various catalytic reactions. In addition, the charge migration distance can be shortened from the inside to the surface which improves the separation efficiency of charges. Low-coordinated atoms with dangling bonds can provide active sites to participate in the catalytic reactions (Di et al., 2018b; Xiong et al., 2018). The thickness-dependent photocatalytic activity toward salicylic acid degradation was reported by Li et al., who prepared the thinner and thicker Bi3O4Cl through the liquid phase exfoliation under isopropanol or further recrystallization (Li J. et al., 2013). The thinnest Bi3O4Cl endows the highest photodegradation activity due to the highest internal electric field. The thinner thickness of Bi24O31Br10 was prepared when a larger amount of NH4Br was used. The higher charge separation efficiency can be realized in thinner Bi24O31Br10 nanosheets, thus leading to the formation of higher reactive oxygen species concentration, favoring the degradation of tetracycline hydrochloride (Wang C. Y. et al., 2017).
Morphology Control
The morphology control is a classic but effective strategy for boosting the photocatalytic activity of BIOX (Garg et al., 2018b; Bárdos et al., 2019; Bárdos et al., 2020). It is well known that porous and hollow solids have excellent adsorptive properties, which is a prerequisite for highly efficiently utilizing photo-induced electron-hole pairs during photocatalysis. BiOI hollow microspheres were synthesized using a facile reactable ionic liquid 1-butyl-3-methylimidazolium iodine ([Bmim]I)-assisted microemulsion method at room temperature (Di et al., 2014). The as-obtained BiOI hollow microspheres shows enhanced photocatalytic activity, which was attributed to the shortened diffusion pathways, lower energy band gap, higher BET surface area, faster interfacial charge transfer rate, and higher separation efficiency of photogenerated electrons and holes. Liu and co-workers prepared the Bi12O17Br2 nanotubes, exhibiting 14.4 times more activity than Bi12O17Br2 nanoplates (Di et al., 2020). The enhanced activity is attributed to better CO2 adsorption and activation, increased carrier separation, and CO desorption, which was induced by the surface tensile strain in Bi12O17Br2 nanotubes.
Bismuth-Rich Strategy
By adjusting the elemental constituents, the energy band structures of BiOX materials can be tuned to meet the requirement of various applications. For example, the bismuth-rich BiOCl and BiOBr can narrow the band gap compared to pristine BiOCl and BiOBr while bismuth-rich BiOI shows an increased band gap (Li J. et al., 2017; Wang Z. et al., 2019). In addition, the bismuth-rich BiOX materials own more abundant tunable surface atomic configurations including surface atomic types, atomic quantity, and atomic distance. Bi24O31Br10 materials display outstanding photocatalytic hydrogen evolution behavior, while the pristine BiOBr has been demonstrated to be inactive for photocatalytic hydrogen evolution (Shang et al., 2014).
Purification of Pollutants and Photocatalyst Recovery
The very positive VB and the modification of BiOX endow photoholes with sufficient thermodynamic energy to be used in organic oxidation. The organics can be degraded directly through hole-oxidation or indirectly by the newly formed oxidative radicals such as hydroxyl radicals (OH−). During this process, the photoelectrons will be removed by dissolved oxygen to maximize the net charge separation efficiency and can also be used to reduce heavy metal ions.
Oxidation Degradation
Photooxidative degradation of many organic pollutants over modified BiOX has been extensively reviewed (Yang et al., 2018; Sharma K. et al., 2019; Garg et al., 2019). Both the decomposition mechanism and the number of intermediates depend on the properties of organic compounds. The abundant organic dyes in textile, apparel, and paper industrial wastewater cause severe environmental pollution. The dye-polluted wastewater carries refractory pigments that are highly harmful and carcinogenic to humans (Brown and De Vito, 1993; Chen et al., 2010). Dyes even at extremely low levels (below 1 ppm) are highly visible in water and severely worsen water environments (Ledakowicz and Gonera, 1999; Grzechulska and Morawski, 2002; Daneshvar et al., 2004). In general, organic dyes are either cationic or anionic according to their chemical structures. Cationic dyes (e.g., RhB, methylene blue, and malachite green) carry cationic functional groups (mostly N+) that can dissociate into cations in aqueous solutions. In contrast, anionic dyes including acid orange 7 and MO contain sulfonic or carboxylic acid groups. Both anionic and cationic functional groups can interact with BiOX with a hydrophilic surface, which is favorable for the oxidation by hole or hydroxyl radicals. For instance, RhB was mainly degraded by hole and hydroxyl radicals in BiOBr/BiOF (Jiang et al., 2017). However, the RhB degradation by BiOBr/TiO2 heterojunction was mediated by superoxide radical anions (O2−), which was produced by single electron reduction of dissolved oxygen (Yang et al., 2021). Organic dye degradation was also investigated using different BiOX-based photocatalysts, namely, BiOCl/CeO2 (Zhang Y. et al., 2020b), W-doped BiOCl (Mokhtari and Tahmasebi, 2021), Bi2WO6/BiOX (X = Cl, Br, I) (Derikvand and Tahmasebi, 2021), and BiVO4/BiOX (X = F, Cl, Br, I) (Razavi-Khosroshahi et al., 2019).
The release of antibacterial agents into the aquatic environment has caused more concerns about their potential environmental risks, especially the occurrence and spread of antibiotic resistance and chronic toxicity to microbial species. Fluoroquinolones (e.g., norfloxacin, ciprofloxacin, moxifloxacin, and ofloxacin) are extensively used as human and veterinary medicine owing to their wide-spectrum activity against Gram- and Gram-negative bacteria (Brain et al., 2004; Liu C. et al., 2012). However, fluoroquinolones cannot be fully metabolised in the body and are largely excreted in their pharmacologically active forms, which make them the most-detected antibiotics in wastewater and surface water (Robinson et al., 2005). In general, the degradation of fluoroquinolones mainly involves amine side-chain degradative oxidation, defluorination, and decarboxylation (Chen and Chu, 2015). Of them, the degradation of the electron-rich amine side-chain to oxidized products is extremely important (Sturini et al., 2012). Different BiOX-based photocatalysts were also designed to reduce antibiotics. For example, Cu2+-doped BiOBr (Lv et al., 2020), Nb5+ -doped BiOBr (Wei et al., 2020), and N-doped BiOCl (Maimaitizi et al., 2020) were used in the degradation of norfloxacin. Type II heterojunctions such as BiVO4/BiOCl (Ma X. et al., 2017), BiOBr/Fe2O3 (Guo et al., 2017), and BiOBr/CdS (Senasu et al., 2021) can reportedly enhance the photodegradation of antibiotics.
Apart from the oxidation degradation of organic dyes and antibiotics, modified BiOX can also be applied to other common organics, including pharmaceutical active compounds (Heidari et al., 2020; Gao et al., 2021) and endocrine-disrupting chemicals (López-Velázquez et al., 2021; Wu et al., 2021; Zhang H. et al., 2021). However, only organics transformation occurs in most cases. Therefore, future works shall focus on the development of modified BiOX with strong oxidation ability to degrade organics and mineralize their byproducts.
Reduction of Heavy Metals
Heavy metal water pollution is a global environmental problem that threatens human health and the ecology. Hexavalent chromium (Cr(VI)) is an essential component in many industrial applications, including electroplating, leather tanning, and anti-corrosion steel, despite its carcinogenicity and mutagenicity (Shi et al., 1994; Salnikow and Zhitkovich, 2008). Compared to other oxidation states of Cr ions, Cr(III) is relatively benign with significantly lower toxicity since it can be excreted from the human body. Hence, photocatalytic reduction of Cr(IV) to Cr(III) is considered as an effective route. Long et al. prepared BiOBr-Bi2S3 heterojunctions via ion-exchange (Long et al., 2021). The performance of photo-reduced Cr(VI) was about 28.9 and 184.6 times higher than those of pure Bi2S3 and BiOBr, respectively. More importantly, the novel composite had a good Cr(III) adsorption efficiency, suggesting that it can be a bifunctional photocatalyst. Similar Cr (VI) removal was also finished with CoFe2O4/BiOBr/graphene, (Li et al., 2019), BiOCl/Bi2S3 (Lu et al., 2020), and BiOClxBr1-x (Hussain et al., 2020). However, there is no example of using BiOX as photocatalysts into the reduction of other heavy metal ions.
Photocatalyst Recovery
Although numerous modified BiOX had been developed and used on photocatalytic degradation, they still faced limitation during the practical application. One of the major challenges that the photocatalysts confront is the inefficient separation and recovery from the aqueous medium after being utilized in the wastewater treatment process. An et al. collected the Cu-doped BiOBr from suspension by centrifuge and then regenerated it by heating at 200°C to remove the residual organic (Lv et al., 2020). Although this method is effective for the recovery of photocatalysts, the process is time consuming and that inevitably raises the treatment cost. The immobilization of photocatalysts on a certain supporting substrate provides a dual advantage; the first is the efficient separation and easy recovery of reused photocatalysts, and the second is the prevention of agglomeration of the photocatalysts for higher photocatalytic performance (Tettey et al., 2010; Cao C. Y. et al., 2012). A wide range of substrates have been employed for the immobilization of BiOX, such as activated carbon, ceramic fibers, and ceramic paper (Yadav et al., 2019; Kása et al., 2020; Yadav et al., 2020). The novel green BiOX (Cl, Br and I) was homogeneously immobilized on Al2O3-based ceramic fiber sheets, which exhibited an excellent photocatalytic performance and recyclability for MO, bisphenol A, and ampicillin disintegration under visible-light irradiation (Yadav et al., 2019).
Summary and Prospects
BiOX-based materials are prospective photocatalysts for environmental treatments, such as waste water remediation, organic pollutant degradation, and heavy metal removal. Therefore, the literature on BiOX (X = Cl, Br, I) was reviewed and discussed to provide some guidance for future studies.
Until now, heat treatments including solvothermal and hydrothermal methods are the most widely used to prepare BiOX. These routes allow researchers to control the morphology, specific surface area, dimension, and pore size and volume. However, this is a time- and energy-consuming process. Therefore, future studies shall focus on a facile method for large-scale synthesis of more attractive BiOBr photocatalysts. The microwave-assisted method allows for the rapid production of BiOX, but the research of this process is still in its infancy.
To boost the activity of BiOX-based semiconductor photocatalysts, researchers are using diverse solutions, such as heterojunction engineering, ion doping, interfacing with carbon materials, coupling with noble metals, and facet control. Although much effort has been dedicated to regulating BiOX-based materials and optimizing their photocatalytic performance, the research in this area is still faced with a lot of challenges, and it is also filled with opportunities. In view of 2D materials, the reduction of atomic layer thickness may bring new properties that the bulk materials do not possess. The layered structure of BiOX enables it to readily form a single layer or few-layer structure. Therefore, researchers may pay attention to control preparation of BiOX with atomic thickness and explore their photocatalytic performance. The defect engineering has been verified to regulate the photocatalytic activity of BiOX, but most of the defect type in BiOX is still oxygen vacancy. More defects have not been constructed in BiOX including halogen vacancies and dual vacancies, which will interact with surface adsorbates during photocatalysis. Furthermore, in the presence of these defects, new electronic states may be induced and affect the electron transfer. Therefore, the investigation of the relationship between defect types and photocatalytic activity is a promising work in the future.
Apart from the modification of BiOX, the exploration of catalytic mechanisms at the atomic level during multiple photocatalytic applications is much needed. The catalytic sites are crucially important and thus it should be determined through calculation or direct experimental observation. More in situ characterization should be performed to gain atomic-level insight into the relationship between active sites and photocatalytic activity, which will guide the design direction of BiOX.
Last, photocatalytic oxidation of organic molecules was reviewed, but most of the works focused on the organic dye degradation at the laboratory scale. However, for practical application of BiOX, the treatment of organics in real water/wastewater is still a challenge, which is mainly due to the existence of dissolved inorganic ions. The photoreduction of heavy metals over BiOX is another important field that shall be investigated in the future. Taking the practical application into consideration, the immobilization techniques for the recovery of material is also important for the development.
Statements
Author contributions
XL prepared and wrote the article, and FL and XH further edited the manuscript and checked the English writing.
Conflict of interest
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
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Summary
Keywords
bismuth oxyhalide, photocatalysis, strategies for photoactivity enhancement, charge separation, wastewater remediation
Citation
Lv X, Lam FLY and Hu X (2022) A Review on Bismuth Oxyhalide (BiOX, X=Cl, Br, I) Based Photocatalysts for Wastewater Remediation. Front. Catal. 2:839072. doi: 10.3389/fctls.2022.839072
Received
19 December 2021
Accepted
10 March 2022
Published
06 April 2022
Volume
2 - 2022
Edited by
Maria Olea, University of Cambridge, United Kingdom
Reviewed by
Jun Di, Nanjing University of Science and Technology, China
Seema Garg, Amity University, India
Updates
Copyright
© 2022 Lv, Lam and Hu.
This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Frank Leung Yuk Lam, kefrank@ust.hk; Xijun Hu, kexhu@ust.hk
This article was submitted to Heterogeneous Catalysis, a section of the journal Frontiers in Catalysis
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