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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Catal.</journal-id>
<journal-title>Frontiers in Catalysis</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Catal.</abbrev-journal-title>
<issn pub-type="epub">2673-7841</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">839072</article-id>
<article-id pub-id-type="doi">10.3389/fctls.2022.839072</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Catalysis</subject>
<subj-group>
<subject>Review</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>A Review on Bismuth Oxyhalide (BiOX, X&#x3d;Cl, Br, I) Based Photocatalysts for Wastewater Remediation</article-title>
<alt-title alt-title-type="left-running-head">Lv et al.</alt-title>
<alt-title alt-title-type="right-running-head">Review Bismuth Oxyhalide Photocatalysts</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Lv</surname>
<given-names>Xincong</given-names>
</name>
<uri xlink:href="https://loop.frontiersin.org/people/1605438/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Lam</surname>
<given-names>Frank Leung Yuk</given-names>
</name>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1427061/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Hu</surname>
<given-names>Xijun</given-names>
</name>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1126198/overview"/>
</contrib>
</contrib-group>
<aff>
<institution>Department of Chemical and Biological Engineering</institution>, <institution>The Hong Kong University of Science and Technology</institution>, <addr-line>Kowloon</addr-line>, <country>Hong Kong SAR, China</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>
<bold>Edited by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1140848/overview">Maria Olea</ext-link>, University of Cambridge, United Kingdom</p>
</fn>
<fn fn-type="edited-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1660712/overview">Jun Di</ext-link>, Nanjing University of Science and Technology, China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1295795/overview">Seema Garg</ext-link>, Amity University, India</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Frank Leung Yuk Lam, <email>kefrank@ust.hk</email>; Xijun Hu, <email>kexhu@ust.hk</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Heterogeneous Catalysis, a section of the journal Frontiers in Catalysis</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>06</day>
<month>04</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="collection">
<year>2022</year>
</pub-date>
<volume>2</volume>
<elocation-id>839072</elocation-id>
<history>
<date date-type="received">
<day>19</day>
<month>12</month>
<year>2021</year>
</date>
<date date-type="accepted">
<day>10</day>
<month>03</month>
<year>2022</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2022 Lv, Lam and Hu.</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Lv, Lam and Hu</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>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.</p>
</license>
</permissions>
<abstract>
<p>Solar energy transformation over semiconductor-based photocatalysis is an ideal solution to environmental problems and future sustainability. Layered bismuth oxyhalides (BiOX, X &#x3d; 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.</p>
</abstract>
<kwd-group>
<kwd>bismuth oxyhalide</kwd>
<kwd>photocatalysis</kwd>
<kwd>strategies for photoactivity enhancement</kwd>
<kwd>charge separation</kwd>
<kwd>wastewater remediation</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="s1">
<title>Introduction</title>
<p>Water pollution and unavailability of clean and inexpensive water are among the biggest challenges of the 21st century (<xref ref-type="bibr" rid="B147">Qu et al., 2013</xref>). Water shortage attacks 1/3 of the global population, and clean drinking water is inaccessible to one billion people (<xref ref-type="bibr" rid="B193">WHO/UNICEF Joint Monitoring Programme for Water Supply and Sanitation and UNICEF, 2005</xref>). 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 (<xref ref-type="bibr" rid="B174">Tollefson, 2011</xref>; <xref ref-type="bibr" rid="B151">Richardson, 2012</xref>; <xref ref-type="bibr" rid="B15">Carlsen et al., 2013</xref>). The existence of emerging contaminants, including toxic heavy metal ions, antibiotics, and endocrine disrupting chemicals (<xref ref-type="bibr" rid="B46">Fatta-Kassinos et al., 2011</xref>; <xref ref-type="bibr" rid="B10">Bueno et al., 2012</xref>), 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 <italic>in situ</italic> formation of largely reactive species (HO&#x2022; and O<sup>2-</sup>&#x2022;) can convert organic contaminants into less harmful substances (e.g., CO<sub>2</sub> and H<sub>2</sub>O) (<xref ref-type="bibr" rid="B88">Lee and Park, 2013</xref>). Various AOPs such as photochemical oxidation (UV/O<sub>3</sub> and UV/H<sub>2</sub>O<sub>2</sub>), chemical oxidation (O<sub>3</sub> and Fenton reagents), and heterogeneous photocatalysis (UV/TiO<sub>2</sub>) (<xref ref-type="bibr" rid="B65">Hidalgo et al., 2007</xref>; <xref ref-type="bibr" rid="B130">Malato et al., 2007</xref>) 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 (<xref ref-type="bibr" rid="B109">Lin et al., 2015</xref>; <xref ref-type="bibr" rid="B86">Landge et al., 2021</xref>). 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 (<xref ref-type="bibr" rid="B63">Herrmann, 1999</xref>; <xref ref-type="bibr" rid="B64">Herrmann, 2005</xref>):<list list-type="simple">
<list-item>
<p>1) mass migration of reactants from the bulk medium to the catalyst&#x2013;fluid interfacial region;</p>
</list-item>
<list-item>
<p>2) surface adsorption of the reactants;</p>
</list-item>
<list-item>
<p>3) photocatalyst activation and surface reaction:</p>
<list list-type="simple">
<list-item>
<p>a absorption of photons by the catalyst</p>
</list-item>
<list-item>
<p>b generation of electron-hole (e<sup>&#x2212;</sup>-h<sup>&#x2b;</sup>) pairs</p>
</list-item>
<list-item>
<p>c diffusion of photogenerated charges to the surface and</p>
</list-item>
<list-item>
<p>d surface transfer of the photocharges to the reactants (i.e., surface reaction)</p>
</list-item>
</list>
</list-item>
<list-item>
<p>4) product desorption from the photocatalyst surface; and</p>
</list-item>
<list-item>
<p>5) mass migration of the products from the interface to the bulk fluid.</p>
</list-item>
</list>
</p>
<p>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 (<xref ref-type="bibr" rid="B66">Hoffmann et al., 1995</xref>). <xref ref-type="fig" rid="F1">Figure 1</xref> displays all the reactions on the catalyst surface mentioned above.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Schematic map of the photocatalysis mechanism over an organic contaminant in water (<xref ref-type="bibr" rid="B110">Linsebigler et al., 1995</xref>).</p>
</caption>
<graphic xlink:href="fctls-02-839072-g001.tif"/>
</fig>
<p>Common photocatalysts (e.g., ZnO and TiO<sub>2</sub>) (<xref ref-type="bibr" rid="B148">Raizada et al., 2016</xref>) mostly can degrade organic pollutants in water under UV irradiation (&#x3c;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 (&#x223c;43% of solar light) with wide pH tolerance and fast division of photocharge carriers are needed. Recently, bismuth-based photocatalysts such as Bi<sub>2</sub>O<sub>3</sub> (<xref ref-type="bibr" rid="B48">Gadhi et al., 2016</xref>; <xref ref-type="bibr" rid="B72">Jalalah et al., 2015</xref>; <xref ref-type="bibr" rid="B139">Oudghiri-Hassani et al., 2015</xref>), Bi<sub>2</sub>WO<sub>6</sub> (<xref ref-type="bibr" rid="B47">Fu et al., 2005</xref>; <xref ref-type="bibr" rid="B231">Zhang and Zhu, 2005</xref>; <xref ref-type="bibr" rid="B236">Zhang et al., 2009</xref>), BiVO<sub>4</sub> (<xref ref-type="bibr" rid="B229">Yu and Kudo, 2006</xref>; <xref ref-type="bibr" rid="B123">Luo et al., 2011</xref>), Bi<sub>2</sub>MoO<sub>6</sub> (<xref ref-type="bibr" rid="B7">Bi et al., 2007</xref>; <xref ref-type="bibr" rid="B237">Zhang et al., 2010</xref>), BiPO<sub>4</sub> (<xref ref-type="bibr" rid="B141">Pan and Zhu, 2011</xref>; <xref ref-type="bibr" rid="B140">Pan and Zhu, 2010</xref>), Bi<sub>2</sub>Ti<sub>2</sub>O<sub>7</sub> (<xref ref-type="bibr" rid="B219">Yao et al., 2004</xref>), (BiO)<sub>2</sub>CO<sub>3</sub> (<xref ref-type="bibr" rid="B136">Ni et al., 2016</xref>), BiOCOOH (<xref ref-type="bibr" rid="B203">Xiong et al., 2011a</xref>), and bismuth oxyhalides (BiOX, X &#x3d; Cl, Br, I) (<xref ref-type="bibr" rid="B62">Henle et al., 2007</xref>; <xref ref-type="bibr" rid="B68">Huang and Zhu, 2008</xref>; <xref ref-type="bibr" rid="B70">Huizhong et al., 2008</xref>; <xref ref-type="bibr" rid="B240">Zhang et al., 2008</xref>; <xref ref-type="bibr" rid="B19">Chang et al., 2010</xref>; <xref ref-type="bibr" rid="B20">Chen et al., 2013</xref>; <xref ref-type="bibr" rid="B27">Cheng et al., 2014</xref>; <xref ref-type="bibr" rid="B220">Ye et al., 2014</xref>; <xref ref-type="bibr" rid="B217">Yang et al., 2018</xref>) have been used in visible-light&#x2013;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/<italic>nmm</italic>). The crystal lattice comprises [Bi<sub>2</sub>O<sub>2</sub>]<sup>2&#x2b;</sup> slice interlayers between halogen anion dual-slabs, gathering along the <italic>z</italic>-axis by the nonbonding (van der Waals) interaction (<xref ref-type="fig" rid="F2">Figure 2A</xref>) (<xref ref-type="bibr" rid="B20">Chen et al., 2013</xref>). This two-dimensional layered structure of BiOX facilitates the formation of an inner electric field between halogen and [Bi<sub>2</sub>O<sub>2</sub>]<sup>2&#x2b;</sup> slabs owing to the transformation of photoexcited electron-hole pairs (<xref ref-type="bibr" rid="B234">Zhang et al., 2006</xref>). The VB of BiOX is constituted by X p (X &#x3d; Cl, Br or I) orbitals and O 2p orbitals (<xref ref-type="bibr" rid="B175">Tu et al., 2012</xref>; <xref ref-type="bibr" rid="B235">Zhang et al., 2012</xref>; <xref ref-type="bibr" rid="B246">Zhao et al., 2013</xref>) while the CB comprises Bi 6p orbitals (<xref ref-type="bibr" rid="B14">Cao J. et al., 2012</xref>; <xref ref-type="bibr" rid="B239">Zhang et al., 2013</xref>). 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 (&#x223c;3.2&#xa0;eV) (<xref ref-type="bibr" rid="B128">Ma Z. et al., 2017</xref>), BiOBr (&#x223c;2.6&#xa0;eV) (<xref ref-type="bibr" rid="B97">Li K. L. et al., 2014</xref>; <xref ref-type="bibr" rid="B85">Kong et al., 2016</xref>), and BiOI (&#x223c;1.8&#xa0;eV) (<xref ref-type="bibr" rid="B201">Xiao and Zhang, 2010</xref>; <xref ref-type="bibr" rid="B221">Ye et al., 2011</xref>) (<xref ref-type="fig" rid="F2">Figure 2B</xref>). Thereby, the light absorbing range can be prolonged from ultraviolet to visible light.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>
<bold>(A)</bold> Crystal structures of BiOX (X &#x3d; Cl, Br, I) (modified with permission (<xref ref-type="bibr" rid="B49">Ganose et al., 2016</xref>)). <bold>(B)</bold> Schematic VB and CB structures of BiOX (data from Ref (<xref ref-type="bibr" rid="B57">Guo et al., 2021</xref>)).</p>
</caption>
<graphic xlink:href="fctls-02-839072-g002.tif"/>
</fig>
<p>In 2006, Zhang <italic>et al.</italic> prepared the BiOCl using the hydrolysis method, and for the first time, they found that BiOCl had a better performance than TiO<sub>2</sub> (P25, Degussa) on photocatalytic degradation of methyl orange (MO) dye (<xref ref-type="bibr" rid="B234">Zhang et al., 2006</xref>). 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 TiO<sub>2</sub> toward MO degradation (<xref ref-type="bibr" rid="B240">Zhang et al., 2008</xref>). In 2015, Ding et al. prepared the BiOCl hierarchical microsphere (2&#x2013;50&#xa0;nm) through controlling pH in the reaction precursor, and the samples showed a preferable photocatalytic activity for rhodamine B (RhB) dye degradation (<xref ref-type="bibr" rid="B45">Ding et al., 2015</xref>). Although BiOCl has better performance than TiO<sub>2</sub>, the large band gap energy (&#x223c;3.2&#xa0;eV) limited their application under visible light.</p>
<p>BiOBr had a narrower band gap (&#x223c;2.6&#xa0;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 (<xref ref-type="bibr" rid="B240">Zhang et al., 2008</xref>). Due to the narrow band gap of BiOBr, it shows 2.5 times and 3.5 times higher catalytic activity than TiO<sub>2</sub> under UV and visible light irradiation. In addition, the flower-like hierarchical architectures of BiOBr was prepared by Jia <italic>et al.</italic>, who employed tetrabutylammonium halide as halogen sources in ethanol solvent (<xref ref-type="bibr" rid="B73">Jia et al., 2015</xref>). The as-obtained BiOBr can degrade rhodamine B and salicylic acid under visible light.</p>
<p>The BiOI owned the narrowest band gap energy (&#x223c;1.8&#xa0;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 (&#x223c;42.6% removal) (<xref ref-type="bibr" rid="B105">Li R. et al., 2015</xref>). Therefore, the BiOI was always used as light harvesting for extending the light adsorption of composites. For example, Zhang et al. prepared the TiO<sub>2</sub>/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 TiO<sub>2</sub> can be improved. As a result, the TiO<sub>2</sub>/BiOI composites show 16.6 times higher methylene blue degradation than TiO<sub>2</sub> (<xref ref-type="bibr" rid="B241">Zhang Y. et al., 2021</xref>).</p>
<p>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 (<xref ref-type="bibr" rid="B57">Guo et al., 2021</xref>). In other words, BiOX can hardly keep responsive light sensitivity, rapid carrier movement, and high redox capability at the same time.</p>
<p>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 Bi<sub>2</sub>WO<sub>6</sub> (<xref ref-type="bibr" rid="B133">Meng and Zhang, 2015</xref>; <xref ref-type="bibr" rid="B199">Xiang et al., 2016</xref>; <xref ref-type="bibr" rid="B181">Wang F. et al., 2018</xref>; <xref ref-type="bibr" rid="B184">Wang J. et al., 2019</xref>; <xref ref-type="bibr" rid="B170">Tahmasebi et al., 2019</xref>), TiO<sub>2</sub> (<xref ref-type="bibr" rid="B143">Park et al., 2012</xref>; <xref ref-type="bibr" rid="B214">Yang J. et al., 2014</xref>; <xref ref-type="bibr" rid="B29">Choi et al., 2016</xref>; <xref ref-type="bibr" rid="B218">Yao et al., 2020</xref>), and Cu<sub>2</sub>O (<xref ref-type="bibr" rid="B12">Cao et al., 2015</xref>; <xref ref-type="bibr" rid="B242">Zhang Y. et al., 2020a</xref>). 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 <italic>via</italic> Schottky contact. The most common decorative metals include platinum (Pt), silver (Ag), and gold (Au) owing to their noble and/or catalytic properties (<xref ref-type="bibr" rid="B224">Yu et al., 2013</xref>; <xref ref-type="bibr" rid="B51">Gao et al., 2014</xref>; <xref ref-type="bibr" rid="B6">Bi et al., 2016</xref>; <xref ref-type="bibr" rid="B114">Liu et al., 2018</xref>; <xref ref-type="bibr" rid="B250">Zhou S. et al., 2019</xref>; <xref ref-type="bibr" rid="B211">Yadav et al., 2021</xref>). 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 (<xref ref-type="bibr" rid="B30">Chou et al., 2016</xref>; <xref ref-type="bibr" rid="B33">Dai and Zhao, 2017</xref>; <xref ref-type="bibr" rid="B89">Lee et al., 2017</xref>; <xref ref-type="bibr" rid="B54">Garg et al., 2018a</xref>; <xref ref-type="bibr" rid="B168">Su et al., 2018</xref>; <xref ref-type="bibr" rid="B157">Sharma N. et al., 2019</xref>; <xref ref-type="bibr" rid="B238">Zhang W. et al., 2019</xref>; <xref ref-type="bibr" rid="B251">Zhu et al., 2019</xref>; <xref ref-type="bibr" rid="B209">Yadav et al., 2020</xref>; <xref ref-type="bibr" rid="B2">Alansi et al., 2021</xref>; <xref ref-type="bibr" rid="B158">Sharma et al., 2022</xref>). 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 (<xref ref-type="bibr" rid="B42">Di et al., 2017</xref>; <xref ref-type="bibr" rid="B92">Li et al., 2018</xref>; <xref ref-type="bibr" rid="B206">Xiong et al., 2020</xref>). However, few studies focus on the intuitive comparison of photocatalytic activity of BiOX prepared by different methods for wastewater treatment.</p>
<p>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.</p>
</sec>
<sec id="s2">
<title>Synthetic Methods of BiOX Photocatalysts</title>
<sec id="s2-1">
<title>Hydro/Solvothermal Method</title>
<p>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 <italic>et al.</italic> prepared BiOBr nanosheets by hydrothermally treating Bi(NO<sub>3</sub>)<sub>3</sub>&#x2219;5H<sub>2</sub>O and KBr at 160&#xb0;C for 12&#xa0;h (<xref ref-type="bibr" rid="B97">Li K. L. et al., 2014</xref>). A similar procedure was extended to the preparation of BiOCl (<xref ref-type="bibr" rid="B204">Xiong et al., 2011b</xref>) and BiOI (<xref ref-type="bibr" rid="B91">Li H. et al., 2013</xref>). Different from the hydrothermal route which uses a precursor water solution, the solvothermal route adopts various solvents (e.g., methanol (<xref ref-type="bibr" rid="B177">Vadivel et al., 2014</xref>), ethylene glycol (<xref ref-type="bibr" rid="B118">Liu et al., 2014</xref>), and glycerol (<xref ref-type="bibr" rid="B117">Liu Z. et al., 2012</xref>)) to synthesize the precursor solution. This route allows the increment of pressure and temperature relative to the hydrothermal route (<xref ref-type="bibr" rid="B117">Liu Z. et al., 2012</xref>). Zhang <italic>et al.</italic> first produced 3D BiOX microspheres by using the solvothermal route with ethylene glycol (<xref ref-type="fig" rid="F3">Figure 3</xref>) (<xref ref-type="bibr" rid="B240">Zhang et al., 2008</xref>) 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&#xb0;C for 5&#xa0;h in a stainless steel vessel (<xref ref-type="bibr" rid="B207">Xiong et al., 2016</xref>). 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.</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>SEM images of BiOCl <bold>(A)</bold>, BiOBr <bold>(B)</bold>, and BiOI microspheres <bold>(C)</bold> (reproduced with permission (<xref ref-type="bibr" rid="B240">Zhang et al., 2008</xref>)).</p>
</caption>
<graphic xlink:href="fctls-02-839072-g003.tif"/>
</fig>
<p>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 (<xref ref-type="bibr" rid="B247">Zhao et al., 2012</xref>). 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 (<xref ref-type="bibr" rid="B132">Mao et al., 2014</xref>).</p>
<p>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&#xa0;m<sup>2</sup>/g surface area <italic>via</italic> the solvothermal procedure using Bi(NO<sub>3</sub>)<sub>3</sub>&#x22c5;5H<sub>2</sub>O, PVP (M &#x3d; 45,000&#x223c;58,000), bromide [C<sub>16</sub>min]Br, and ethylene glycol as precursors while keeping the reaction at 140&#xb0;C for 24&#xa0;h (<xref ref-type="bibr" rid="B116">Liu and Wu, 2017</xref>). Hao <italic>et al.</italic> compared the effect of PVP on BiOI photocatalytic activity (<xref ref-type="bibr" rid="B59">Hao et al., 2012</xref>). 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%).</p>
</sec>
<sec id="s2-2">
<title>Alcoholysis/Hydrolysis</title>
<p>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&#xa0;h of BiCl<sub>3</sub> hydrolysis at 65&#xb0;C using acetylacetone as an assisting solvent under acidic conditions (<xref ref-type="bibr" rid="B3">Armelao et al., 2012</xref>). Song et al. prepared 21- to 85-nm-thick BiOCl nanosheets from hydrolysis of Bi(NO<sub>3</sub>)<sub>3</sub> with HCl and Na<sub>2</sub>CO<sub>3</sub> by keeping it at &#x223c; pH2 for 30&#xa0;min at ambient temperature (<xref ref-type="bibr" rid="B164">Song et al., 2017</xref>). Zhang et al. compared the photocatalytic activity of BiOBr prepared by hydrolysis and alcoholysis and added 0.5&#xa0;g of BiBr<sub>3</sub> to 15&#xa0;ml of solvent of water or isopropyl alcohol at room temperature (<xref ref-type="bibr" rid="B101">Li R. et al., 2015</xref>). Then the suspension was heated at 20, 40, or 60&#xb0;C for 10&#xa0;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 (<xref ref-type="fig" rid="F4">Figure 4</xref>) (<xref ref-type="bibr" rid="B58">Han et al., 2020</xref>) Different bismuth or bromine sources, solvents, capping agents, or surfactants affected the morphology of BiOBr during hydrolysis. The direct hydrolysis of BiI<sub>3</sub> was used to prepare BiOI by Su et al., who used the as-obtained BiOI to degrade Rhodamine B under simulated solar light (<xref ref-type="bibr" rid="B166">Su et al., 2014</xref>).</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>Schematic map of the probable formation of 0D, 1D, 2D, or 3D BiOBr (Modified from Ref (<xref ref-type="bibr" rid="B58">Han et al., 2020</xref>)).</p>
</caption>
<graphic xlink:href="fctls-02-839072-g004.tif"/>
</fig>
</sec>
<sec id="s2-3">
<title>Template Method</title>
<p>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 (<xref ref-type="bibr" rid="B202">Xie et al., 2016</xref>). 1) A template is produced. 2) The target product is synthesized under the action of the template <italic>via</italic> 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 Bi<sup>3&#x2b;</sup> and Cl<sup>&#x2212;</sup>, followed by sintering up to 400&#xb0;C to form hollow BiOCl microspheres, which were in a shell thickness of 40&#xa0;nm and a diameter of 200&#xa0;nm (<xref ref-type="bibr" rid="B32">Cui et al., 2016</xref>). With a butterfly wing as a biological template, Yan et al. prepared hierarchical BiOCl (<xref ref-type="bibr" rid="B212">Yan et al., 2019</xref>). BiOI was also used as a self-sacrifice template to construct Bi<sub>4</sub>O<sub>5</sub>I<sub>2</sub>/Bi<sub>5</sub>O<sub>7</sub>I and BiOI/Bi<sub>4</sub>O<sub>5</sub>I<sub>2</sub> heterojunctions from simple calcination (<xref ref-type="bibr" rid="B28">Cheng et al., 2020</xref>). The BiOBr self-sacrifice template was also used for the formation of BiOBr/Bi<sub>4</sub>O<sub>5</sub>Br<sub>2</sub> (<xref ref-type="bibr" rid="B100">Li P. et al., 2020</xref>).</p>
</sec>
<sec id="s2-4">
<title>Other Methods</title>
<p>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&#xa0;min of microwave processing (<xref ref-type="bibr" rid="B90">Li et al., 2012</xref>). The BiOBr showed a Brunauer, Emmett and Teller (BET) surface area of 63.5&#xa0;m<sup>2</sup>/g and an outstanding removal ability and fast adsorbing rate over Cr<sup>6&#x2b;</sup> in a wide pH range. Reportedly, the presence of surfactants during microwave processing improved the BiOBr photocatalytic activity (<xref ref-type="bibr" rid="B26">Chen et al., 2017</xref>). 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) (<xref ref-type="bibr" rid="B60">He et al., 2015</xref>). 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 (<xref ref-type="bibr" rid="B1">Ai et al., 2014</xref>).</p>
<p>During preparation of BiOBr by co-precipitation (<xref ref-type="bibr" rid="B121">Lu et al., 2012</xref>), Bi(NO<sub>3</sub>)<sub>3</sub> and KBr were mixed in acetic acid water solution, stirred, and aged for 6&#xa0;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 (<xref ref-type="bibr" rid="B185">Wang and Zhang, 2020</xref>). 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 (&#x223c;47.5&#xa0;m<sup>2</sup>&#xa0;g<sup>&#x2212;1</sup>) and thus had an excellent photocatalytic activity for NO removal (98%) in the gaseous phase (<xref ref-type="bibr" rid="B135">Montoya-Zamora et al., 2017</xref>).</p>
<p>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 Bi<sub>24</sub>O<sub>31</sub>Br<sub>10</sub> was prepared <italic>via</italic> sintering of BiOBr at 750&#xb0;C (<xref ref-type="bibr" rid="B226">Yu C. et al., 2012</xref>). A similar process was extended to the synthesis of hollow Bi<sub>24</sub>O<sub>31</sub>Cl<sub>10</sub> microspheres at 600&#xb0;C (<xref ref-type="bibr" rid="B32">Cui et al., 2016</xref>). The 3D hierarchical bismuth oxyiodides was prepared using the ethylene glycol&#x2013;assisted <italic>in situ</italic> 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&#xa0;nm in an orderly manner, rendering the adjustable oxidation and reduction ability of band energy levels (<xref ref-type="bibr" rid="B67">Huang et al., 2017</xref>).</p>
</sec>
</sec>
<sec id="s3">
<title>Various Techniques to Improve Photocatalytic Activity of BiOX</title>
<p>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 (&#x223c;3.22&#xa0;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.</p>
<sec id="s3-1">
<title>Heterojunction</title>
<p>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 (<xref ref-type="bibr" rid="B213">Yang, 2021</xref>). 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 (<xref ref-type="fig" rid="F5">Figure 5A</xref>). 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 (<xref ref-type="bibr" rid="B137">Ning et al., 2016</xref>). Yang et al. prepared type II Bi<sub>2</sub>WO<sub>6</sub>/BiOBr heterojunction <italic>via</italic> a one-step solvothermal route for degradation of rhodamine B (RhB), methylene blue, and colorless TCHC (<xref ref-type="fig" rid="F6">Figure 6A</xref>) (<xref ref-type="bibr" rid="B150">Ren et al., 2019</xref>) Guo et al. prepared BiVO<sub>4</sub>/BiOCl heterojunction with a higher charge separation rate than pure BiVO<sub>4</sub> or BiOCl (<xref ref-type="bibr" rid="B112">Liu et al., 2019</xref>). More research on BiOX-based Type II heterojunction can be found in <xref ref-type="table" rid="T1">Table 1</xref>.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>
<bold>(A)</bold> Type II photocatalysts; <bold>(B)</bold> p-n junction; and <bold>(C)</bold> Z-scheme strategy for higher photocatalytic activity.</p>
</caption>
<graphic xlink:href="fctls-02-839072-g005.tif"/>
</fig>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>
<bold>(A)</bold> Photocatalytic mechanism of pollution by Bi<sub>2</sub>WO<sub>6</sub>/BiOBr catalyst (Type II heterojunction) (<xref ref-type="bibr" rid="B150">Ren et al., 2019</xref>). <bold>(B)</bold> Diagram of BiOBr/SnO<sub>2</sub> p-n heterojunction charge transfer at the interface, electron location function, and charge difference distribution (<xref ref-type="bibr" rid="B195">Wu et al., 2020</xref>); <bold>(C)</bold> Charge transfer in Z-scheme CdS/BiOCl catalyst (<xref ref-type="bibr" rid="B171">Tang et al., 2020</xref>).</p>
</caption>
<graphic xlink:href="fctls-02-839072-g006.tif"/>
</fig>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Summary of BiOX-based composites with improved photocatalytic activity.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Photocatalysts</th>
<th align="center">Synthesis method</th>
<th align="center">Light source</th>
<th align="center">Improved performances</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td colspan="4" align="left">
<italic>Heterojunction</italic>
</td>
</tr>
<tr>
<td align="left">&#x2003;Bi<sub>2</sub>WO<sub>6</sub>/BiOBr (<xref ref-type="bibr" rid="B150">Ren et al., 2019</xref>) (Type II)</td>
<td align="left">Solvothermal</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">12 times that of BiOBr and 23 times that of Bi<sub>2</sub>WO<sub>6</sub> for RhB degradation in 60&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;S-C<sub>3</sub>N<sub>4</sub>/BiOBr (<xref ref-type="bibr" rid="B178">Vinoth and Pandikumar, 2021</xref>) (Type II)</td>
<td align="left">Ultrasonic hydrothermal</td>
<td align="left">AM 1.5G, 100&#xa0;mW/cm<sup>2</sup>
</td>
<td align="left">13 times that of BiOBr and 89 times that of S-gC<sub>3</sub>N<sub>4</sub> for PEC water oxidation</td>
</tr>
<tr>
<td align="left">&#x2003;Bi<sub>2</sub>SiO<sub>5</sub>/BiOBr (<xref ref-type="bibr" rid="B16">Chai et al., 2019</xref>) (Type II)</td>
<td align="left">Ion exchange</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">1,253 times that of BiOBr and 25.2 times that of BiVO<sub>4</sub> for RhB degradation in 90&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;BiVO<sub>4</sub>/BiOCl (<xref ref-type="bibr" rid="B112">Liu et al., 2019</xref>) (Type II)</td>
<td align="left">Ion exchange</td>
<td align="left">AM 1.5G, 100&#xa0;mW/cm<sup>2</sup>
</td>
<td align="left">102 times that of BiOCl and 1.44 times that of BiVO<sub>4</sub> for PEC water splitting</td>
</tr>
<tr>
<td align="left">&#x2003;Bi<sub>2</sub>S<sub>3</sub>/BiOCl (<xref ref-type="bibr" rid="B188">Wang Y. et al., 2018</xref>) (Type II)</td>
<td align="left">Epitaxial growth</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm, 100&#xa0;mW/cm<sup>2</sup>
</td>
<td align="left">15 times that of BiOCl and 2 times that of Bi<sub>2</sub>S<sub>3</sub> for PEC water splitting</td>
</tr>
<tr>
<td align="left">&#x2003;CeO<sub>2</sub>/BiOCl (<xref ref-type="bibr" rid="B182">Wang H. et al., 2020</xref>) (Type II)</td>
<td align="left">Precipitation hydrothermal</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">1.67 times that of BiOCl and 3.37 times that of CeO<sub>2</sub> for methyl tetracycline degradation in 120&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;g-C<sub>3</sub>N<sub>4</sub>/BiOI (<xref ref-type="bibr" rid="B179">Vinoth et al., 2021</xref>) (Type II)</td>
<td align="left">Ultrasonic hydrothermal</td>
<td align="left">AM 1.5G, 100&#xa0;mW/cm<sup>2</sup>
</td>
<td align="left">2 times that of BiOI and 11 times that of g-C<sub>3</sub>N<sub>4</sub> for PEC water splitting</td>
</tr>
<tr>
<td align="left">&#x2003;SnS/BiOI (<xref ref-type="bibr" rid="B83">Juntrapirom et al., 2017</xref>) (Type II)</td>
<td align="left">Hydrothermal coprecipitation</td>
<td align="left">&#x3bb; &#x2265; 400&#xa0;nm (50&#xa0;W Hg lamp)</td>
<td align="left">1.67 times that of BiOI and 4.97 times that of SnS for MO degradation in 60&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;BiOBr/Bi<sub>2</sub>O<sub>2</sub>CO<sub>3</sub> (<xref ref-type="bibr" rid="B183">Wang J. J. et al., 2020</xref>) (p-n junction)</td>
<td align="left">Precipitation conversion</td>
<td align="left">300&#xa0;W Xe lamp</td>
<td align="left">14.7 times that of Bi<sub>2</sub>O<sub>2</sub>CO<sub>3</sub> and 4.03 times that of BiOBr for RhB degradation in 20&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;BiOBr/SnO<sub>2</sub> (<xref ref-type="bibr" rid="B195">Wu et al., 2020</xref>) (p-n junction)</td>
<td align="left">Hydrothermal</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (150&#xa0;W Xe lamp)</td>
<td align="left">1.5 times that of BiOBr and 12.2 times that of SnO<sub>2</sub> for NO removal in 5&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;BiPO<sub>4</sub>/BiOCl (<xref ref-type="bibr" rid="B232">Zhang Z. et al., 2020</xref>) (p-n junction)</td>
<td align="left">
<italic>In situ</italic> chemical transformation</td>
<td align="left">300&#xa0;W xenon lamp</td>
<td align="left">3.18 times that of BiOCl for RhB degradation in 90&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;BiOI/g-C<sub>3</sub>N<sub>4</sub> (<xref ref-type="bibr" rid="B173">Tian et al., 2020</xref>) (p-n junction)</td>
<td align="left">Precipitation</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">10 times that of g-C3N4 and 4 times that of BiOI for bisphenol A degradation in 4&#xa0;h</td>
</tr>
<tr>
<td align="left">&#x2003;TiO<sub>2</sub>/BiOI (<xref ref-type="bibr" rid="B241">Zhang Y. et al., 2021</xref>) (p-n junction)</td>
<td align="left">Hydrothermal</td>
<td align="left">Visible light, 300&#xa0;mW/cm<sup>2</sup>
</td>
<td align="left">16.6 times that of TiO<sub>2</sub> and 1.38 times that of BiOI for methylene blue degradation in 60&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;BiOI/ZnO (<xref ref-type="bibr" rid="B200">Xiao et al., 2020</xref>) (p-n junction)</td>
<td align="left">Hydrothermal</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">9.2 times that of BiOI and 2 times that of ZnO for methylene blue degradation in 180&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;CDs/BiOCl (<xref ref-type="bibr" rid="B108">Lin et al., 2017</xref>) (Z-scheme)</td>
<td align="left">Electrochemical</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (350&#xa0;W Xe lamp)</td>
<td align="left">7.62 times that of BiOCl for RhB degradation in 180&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;BiOBr/MnFe<sub>2</sub>O<sub>4</sub> (<xref ref-type="bibr" rid="B162">Sin et al., 2020</xref>) (Z-scheme)</td>
<td align="left">Hydrothermal</td>
<td align="left">Visible light (105&#xa0;W compact fluorescent lamp)</td>
<td align="left">2.85 times that of BiOBr and 6.42 times that of MnFe<sub>2</sub>O<sub>4</sub> for RhB degradation in 80&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;BiOBr/BiOIO<sub>3</sub> (<xref ref-type="bibr" rid="B74">Jia et al., 2020a</xref>) (Z-scheme)</td>
<td align="left">Solvothermal</td>
<td align="left">&#x3bb; &#x3c; 400&#xa0;nm (9&#xa0;W LED light)</td>
<td align="left">1.24 times that of BiOIO<sub>3</sub> and 4.42 times that of BiOBr for removal of heavy metal mercury in 60&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;BiOBr/Bi<sub>2</sub>MoO<sub>6</sub> (<xref ref-type="bibr" rid="B187">Wang S. et al., 2017</xref>) (Z-scheme)</td>
<td align="left">Two-step coprecipitation</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">10.0 times that of pure BiOBr and 54.5 times that of pure Bi<sub>2</sub>MoO<sub>6</sub> for RhB degradation in 25&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;AgI/BiOBr (<xref ref-type="bibr" rid="B228">Yu et al., 2018</xref>) (Z-scheme)</td>
<td align="left">Solvothermal precipitation</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">2.75 times that of BiOBr and 52.5 times that of AgI for ciprofloxacin degradation in 60&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;SnNb<sub>2</sub>O<sub>6</sub>/BiOCl (<xref ref-type="bibr" rid="B80">Jiang et al., 2019</xref>) (Z-scheme)</td>
<td align="left">Two-step hydrothermal</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (250&#xa0;W Xe lamp)</td>
<td align="left">10.51 times that of SnNb<sub>2</sub>O<sub>6</sub> and 20.58 times that of BiOCl for benzocaine degradation in 90&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;BiOCl/g-C<sub>3</sub>N<sub>4</sub> (<xref ref-type="bibr" rid="B169">Sun et al., 2020</xref>) (Z-scheme)</td>
<td align="left">Hydrothermal</td>
<td align="left">Simulated solar light (300&#xa0;W Xe lamp)</td>
<td align="left">20.51 times that of BiOCl for tetracycline degradation in 60&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;BiOI/Bi<sub>2</sub>O<sub>4</sub> (<xref ref-type="bibr" rid="B146">Qin et al., 2020</xref>) (Z-scheme)</td>
<td align="left">Ultrasonic hydrothermal</td>
<td align="left">100&#xa0;W LED lamp</td>
<td align="left">2.81 times that of Bi<sub>2</sub>O<sub>4</sub> and 30 times that of BiOI for RhB degradation in 32&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;Co<sub>3</sub>O<sub>4</sub>/BiOI (<xref ref-type="bibr" rid="B131">Malefane et al., 2020</xref>) (Z-scheme)</td>
<td align="left">Solvothermal</td>
<td align="left">60&#xa0;W LED lamp</td>
<td align="left">80.1 times that of Co<sub>3</sub>O<sub>4</sub> and 13.5 times that of BiOI for ibuprofen degradation in 60&#xa0;min</td>
</tr>
<tr>
<td colspan="4" align="left">
<italic>Elemental doping</italic>
</td>
</tr>
<tr>
<td align="left">&#x2003;Cu<sup>2&#x2b;</sup>-doped BiOBr (<xref ref-type="bibr" rid="B124">Lv et al., 2020</xref>)</td>
<td align="left">Solvothermal</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">2.28 times higher than that of undoped BiOBr for norfloxacin degradation in 90&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;Zn<sup>2&#x2b;</sup>-doped BiOBr (<xref ref-type="bibr" rid="B249">Zhou J. et al., 2019</xref>)</td>
<td align="left">Solvothermal</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">3.35 times enhancement for the RhB degradation in 30&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;Ag/Ti-doped BiOBr (<xref ref-type="bibr" rid="B77">Jiang G. et al., 2012</xref>)</td>
<td align="left">Solvothermal reduction</td>
<td align="left">&#x3bb; &#x2265; 400&#xa0;nm (11&#xa0;W daylight lamp)</td>
<td align="left">5.11 times enhancement for the RhB degradation in 30&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;Sn<sup>2&#x2b;</sup>-doped BiOBr (<xref ref-type="bibr" rid="B176">Tu et al., 2015</xref>)</td>
<td align="left">Solvothermal</td>
<td align="left">Visible light (500&#xa0;W Xe lamp)</td>
<td align="left">2.71 times higher than pure BiOBr for RhB degradation in 16&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;Zn<sup>2&#x2b;</sup>-doped BiOCl (<xref ref-type="bibr" rid="B102">Li W. T. et al., 2015</xref>)</td>
<td align="left">Solvothermal</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">2.71 times higher than pure BiOCl for the RhB degradation in 60&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;Mn<sup>3&#x2b;</sup>-doped BiOCl (<xref ref-type="bibr" rid="B142">Pare et al., 2011</xref>)</td>
<td align="left">Hydrolysis</td>
<td align="left">Visible light (500&#xa0;W halogen lamp)</td>
<td align="left">1.53 times improvement for malachite green photodegradation in 180&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;N-doped BiOBr (<xref ref-type="bibr" rid="B120">L&#xf3;pez-Vel&#xe1;zquez et al., 2021</xref>)</td>
<td align="left">Microwave-assisted solvothermal</td>
<td align="left">300&#x2013;800&#xa0;nm with an intensity of 30&#xa0;W/m<sup>2</sup> in the UV region</td>
<td align="left">3.3, 2.2, 4.1, and 1.4 times improvement for bisphenol A, 17&#x3b2;-estradiol, 17&#x3b1;-ethinylestradiol, and 4-tert-octylphenol photodegradation, respectively</td>
</tr>
<tr>
<td align="left">&#x2003;P-doped BiOI (<xref ref-type="bibr" rid="B126">Ma F.Q. et al., 2017</xref>)</td>
<td align="left">Hydrothermal</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">2.63 times higher than BiOI for RhB degradation in 60&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;C-doped BiOBr (<xref ref-type="bibr" rid="B244">Zhang W. et al., 2019</xref>)</td>
<td align="left">Hydrothermal</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (800&#xa0;W Xe lamp)</td>
<td align="left">4.7 times enhancement for tetracycline degradation in 25&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;S-doped BiOBr (<xref ref-type="bibr" rid="B115">Liu et al., 2021</xref>)</td>
<td align="left">Solvothermal</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">3 times higher than pure BiOBr for ibuprofen degradation in 240&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;La<sup>3&#x2b;</sup>-doped BiOBr (<xref ref-type="bibr" rid="B222">Yin et al., 2017</xref>)</td>
<td align="left">Solvothermal</td>
<td align="left">&#x3bb; &#x2265; 400&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">3.8 and 1.7 times enhancement for RhB in 60&#xa0;min and ciprofloxacin in 180&#xa0;min degradation, respectively</td>
</tr>
<tr>
<td align="left">&#x2003;Y<sup>3&#x2b;</sup>-doped BiOCl (<xref ref-type="bibr" rid="B248">Zhong et al., 2020</xref>)</td>
<td align="left">Consecutive solvent-based and thermal</td>
<td align="left">Visible light (300&#xa0;W xenon lamp)</td>
<td align="left">1.8 times improvement for the tetracycline hydrochloride within 90&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;Er ion&#x2013;doped BiOBr (<xref ref-type="bibr" rid="B198">Xia et al., 2016</xref>)</td>
<td align="left">Solvothermal</td>
<td align="left">&#x3bb; &#x2265; 400&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">1.8-fold improvement for ciprofloxacin degradation within 360&#xa0;min</td>
</tr>
<tr>
<td colspan="4" align="left">
<italic>Noble metal deposition</italic>
</td>
</tr>
<tr>
<td align="left">&#x2003;Ag/BiOBr (<xref ref-type="bibr" rid="B225">Yu et al., 2011</xref>)</td>
<td align="left">Photodeposition</td>
<td align="left">Visible light (300-W tungsten lamp)</td>
<td align="left">14-fold improvement for acid orange II degradation in 40&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;Pd/BiOBr (<xref ref-type="bibr" rid="B104">Li X. et al., 2020</xref>)</td>
<td align="left">Photodeposition</td>
<td align="left">Xe lamp at 200&#xa0;mW&#xa0;cm<sup>&#x2212;2</sup>
</td>
<td align="left">1.5 times improvement for photocatalytic selective oxidation of toluene to benzaldehyde</td>
</tr>
<tr>
<td align="left">&#x2003;Rh, Pd, Pt/BiOCl (<xref ref-type="bibr" rid="B224">Yu et al., 2013</xref>)</td>
<td align="left">Photodeposition</td>
<td align="left">420&#xa0;nm &#x3c; &#x3bb; &#x3c; 660&#xa0;nm (150&#xa0;W tungsten halogen lamp)</td>
<td align="left">2.1, 2.2, and 3.1 times enhancement for Rh, Pd, and Pt deposited BiOCl for acid orange II degradation</td>
</tr>
<tr>
<td align="left">&#x2003;Ag/BiOCl (<xref ref-type="bibr" rid="B227">Yu et al., 2017</xref>)</td>
<td align="left">Photodeposition</td>
<td align="left">Two 365&#xa0;nm LED lamps with an average light intensity of 80&#xa0;mW&#xa0;cm<sup>&#x2212;2</sup>
</td>
<td align="left">2.5-fold improvement for MO degradation</td>
</tr>
<tr>
<td align="left">&#x2003;Pd/BiOCl (<xref ref-type="bibr" rid="B24">Chen et al., 2014</xref>)</td>
<td align="left">Solvothermal</td>
<td align="left">Visible light (300&#xa0;W Xe lamp)</td>
<td align="left">2.5-fold enhancement for RhB degradation</td>
</tr>
<tr>
<td align="left">&#x2003;Au/BiOI (<xref ref-type="bibr" rid="B17">Chang et al., 2021</xref>)</td>
<td align="left">Ion sputter</td>
<td align="left">AM 1.5G at 100&#xa0;mW/cm<sup>2</sup> (300&#xa0;W Xe lamp)</td>
<td align="left">24-fold improvement in PEC efficiency over bare BiOI</td>
</tr>
<tr>
<td align="left">&#x2003;Ag/BiOI (<xref ref-type="bibr" rid="B113">Liu H. et al., 2012</xref>)</td>
<td align="left">Hydrothermal and photodeposition</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (500&#xa0;W Xe lamp)</td>
<td align="left">4.00, 3.99, and 3.39 times improvement over BiOI in degradation of acid orange II, MO, and RhB, respectively</td>
</tr>
<tr>
<td colspan="4" align="left">
<italic>Interfacing with carbon materials</italic>
</td>
</tr>
<tr>
<td align="left">&#x2003;BiOBr/graphene (<xref ref-type="bibr" rid="B175">Tu et al., 2012</xref>)</td>
<td align="left">EG-assisted solvothermal</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (500&#xa0;W Xe lamp)</td>
<td align="left">3 times higher than BiOBr for RhB degradation</td>
</tr>
<tr>
<td align="left">&#x2003;BiOBr/graphene hydrogel (<xref ref-type="bibr" rid="B18">Chang et al., 2020</xref>)</td>
<td align="left">Two-step hydrothermal</td>
<td align="left">Visible light (300&#xa0;W Xe lamp)</td>
<td align="left">1.83 times higher than that of BiOBr for degradation of potassium butyl xanthate</td>
</tr>
<tr>
<td align="left">&#x2003;BiOCl/graphene (<xref ref-type="bibr" rid="B106">Li Z. et al., 2017</xref>)</td>
<td align="left">Hydrothermal</td>
<td align="left">Full arc (150&#xa0;W Xe lamp)</td>
<td align="left">8.4 and 3.8 times higher than BiOCl for degradation of MO and oxidation of water</td>
</tr>
<tr>
<td align="left">&#x2003;GO foam/BiOI</td>
<td align="left">
<italic>In situ</italic> deposition</td>
<td align="left">&#x3bb; &#x2265; 400&#xa0;nm (60&#xa0;W LED spotlight lamp)</td>
<td align="left">1.84 times improvement for phenol degradation in 150&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;BiOI/CNT (<xref ref-type="bibr" rid="B159">Sharma et al., 2021</xref>)</td>
<td align="left">Hydrothermal</td>
<td align="left">Visible light (4 &#xd7; 24&#xa0;W visible light lamps)</td>
<td align="left">2 times and 3 times higher than BiOI for degradation of phenol and RhB</td>
</tr>
<tr>
<td align="left">&#x2003;BiOI-MWCNT (<xref ref-type="bibr" rid="B167">Su et al., 2012</xref>)</td>
<td align="left">EG-assisted solvothermal</td>
<td align="left">&#x3bb; &#x2265; 400&#xa0;nm (150&#xa0;W Xe lamp)</td>
<td align="left">2.1 times higher than BiOI for degradation of acid orange II in 180&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;BiOCl-carbon quantum dots (<xref ref-type="bibr" rid="B41">Di et al., 2015</xref>)</td>
<td align="left">Mannitol-assisted solvothermal</td>
<td align="left">&#x3bb; &#x2265; 400&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">2.22 and 2.12 times higher than pure BiOCl for the degradation of RhB in 40&#xa0;min and degradation of BPA in 120&#xa0;min</td>
</tr>
<tr>
<td colspan="4" align="left">
<italic>Defect engineering</italic>
</td>
</tr>
<tr>
<td align="left">&#x2003;BiOBr-OV (<xref ref-type="bibr" rid="B93">Li H. et al., 2015</xref>)</td>
<td align="left">EG-assisted solvothermal</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (LED light, 10&#xa0;W/cm<sup>2</sup>)</td>
<td align="left">Can generate NH<sub>3</sub> under light irradiation versus BiOBr without OV</td>
</tr>
<tr>
<td align="left">&#x2003;BiOBr-OV (<xref ref-type="bibr" rid="B125">Lyu et al., 2019</xref>)</td>
<td align="left">Solvothermal</td>
<td align="left">Full arc (10&#xa0;W LED lamp)</td>
<td align="left">3.5 times improvement for tetracycline degradation over BiOBr</td>
</tr>
<tr>
<td align="left">&#x2003;OV-rich S-doped BiOBr (<xref ref-type="bibr" rid="B186">Wang Q. et al., 2019</xref>)</td>
<td align="left">Solvothermal</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">4.9 and 18.0 times those of pristine BiOBr and OV-poor S-doped BiOBr for 4-CP degradation within 120&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;BiOBr-OV (<xref ref-type="bibr" rid="B161">Shi et al., 2018</xref>)</td>
<td align="left">Solvothermal</td>
<td align="left">Visible light (300&#xa0;W Xe lamp)</td>
<td align="left">3, 2.69, 2, and 1.74 times improvement for degradation of phenol, BPA, RhB, and MO compared with OV-poor BiOBr, respectively</td>
</tr>
<tr>
<td align="left">&#x2003;BiO<sub>1&#x2212;x</sub>Cl (<xref ref-type="bibr" rid="B13">Cao et al., 2018</xref>)</td>
<td align="left">Diethylene glycol solvothermal</td>
<td align="left">&#x3bb; &#x2265; 400&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">Adsorbing 42% ciprofloxacin and 40% doxycycline, no adsorption on BiOCl; degrading ciprofloxacin and doxycycline after 40 min, only 30% removal over BiOCl</td>
</tr>
<tr>
<td align="left">&#x2003;BiOCl-OV (<xref ref-type="bibr" rid="B163">Song et al., 2021</xref>)</td>
<td align="left">Sodium dodecylbenzenesulfonate hydrothermal</td>
<td align="left">&#x3bb; &#x2265; 400&#xa0;nm (Xe lamp)</td>
<td align="left">1.48 times improvement for the oxytetracycline hydrochloride degradation</td>
</tr>
<tr>
<td align="left">&#x2003;BiOCl-OV (<xref ref-type="bibr" rid="B31">Cui et al., 2018</xref>)</td>
<td align="left">Solvothermal</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">3.3 times higher for oxygen evolution than OV-poor BiOCl</td>
</tr>
<tr>
<td align="left">&#x2003;BiOI-OV (<xref ref-type="bibr" rid="B69">Huang et al., 2014</xref>)</td>
<td align="left">Solvothermal</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (500&#xa0;W Xe lamp)</td>
<td align="left">1 order-of-magnitude improvement in donor density versus BiOI and 10 times higher photocatalytic activity than BiOI for MO degradation</td>
</tr>
<tr>
<td align="left">&#x2003;BiOI-OV (<xref ref-type="bibr" rid="B25">Chen et al., 2016</xref>)</td>
<td align="left">Glycerol solvothermal</td>
<td align="left">Visible light (300&#xa0;W Xe lamp)</td>
<td align="left">3.5 times higher than untreated BiOI nanosheets for MO degradation</td>
</tr>
<tr>
<td colspan="4" align="left">
<italic>Facet control</italic>
</td>
</tr>
<tr>
<td align="left">&#x2003;BiOBr-110 (<xref ref-type="bibr" rid="B144">Peng et al., 2017</xref>)</td>
<td align="left">Glucose hydrothermal</td>
<td align="left">&#x3bb; &#x2265; 400&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">Degrading 91% MO in 30 min and 100% RhB in 10 min, 60% MO and 70% RhB by BiOBr-001</td>
</tr>
<tr>
<td align="left">&#x2003;BiOBr-010 (<xref ref-type="bibr" rid="B197">Wu et al., 2017</xref>)</td>
<td align="left">Chemical precipitation</td>
<td align="left">Visible light (300&#xa0;W Xe lamp)</td>
<td align="left">3 times improvement of PEC performance over BiOBr-001</td>
</tr>
<tr>
<td align="left">&#x2003;BiOBr-010 (<xref ref-type="bibr" rid="B75">Jia et al., 2020b</xref>)</td>
<td align="left">pH adjustment</td>
<td align="left">&#x3bb; &#x3c; 420&#xa0;nm (9&#xa0;W LED lamp)</td>
<td align="left">1.2 times improvement for Hg oxidation over BiOBr-001</td>
</tr>
<tr>
<td align="left">&#x2003;BiOCl-001, BiOCl-010 (<xref ref-type="bibr" rid="B78">Jiang J. et al., 2012</xref>)</td>
<td align="left">Hydrothermal</td>
<td align="left">UV or visible light (300&#xa0;W Xe lamp)</td>
<td align="left">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</td>
</tr>
<tr>
<td colspan="4" align="left">
<italic>Thickness tuning</italic>
</td>
</tr>
<tr>
<td align="left">&#x2003;Thickness-controllable Bi<sub>24</sub>O<sub>31</sub>Br<sub>10</sub> nanosheets (<xref ref-type="bibr" rid="B180">Wang C. Y. et al., 2017</xref>)</td>
<td align="left">NH<sub>4</sub>Br hydrothermal</td>
<td align="left">&#x3bb; &#x2265; 420&#xa0;nm (520&#xa0;W Xe lamp)</td>
<td align="left">Bi<sub>24</sub>O<sub>31</sub>Br<sub>10</sub> (&#x223c;40&#xa0;nm thickness) is 3.11 and 4.79 times higher than that of Bi<sub>24</sub>O<sub>31</sub>Br<sub>10</sub> with 80&#xa0;nm and with 130&#xa0;nm thickness for tetracycline hydrochloride degradation</td>
</tr>
<tr>
<td colspan="4" align="left">
<italic>Morphology control</italic>
</td>
</tr>
<tr>
<td align="left">&#x2003;BiOI hollow microspheres (<xref ref-type="bibr" rid="B39">Di et al., 2014</xref>)</td>
<td align="left">Ionic liquid-assisted microemulsion method</td>
<td align="left">&#x3bb; &#x2265; 400&#xa0;nm (300&#xa0;W Xe lamp)</td>
<td align="left">BiOI hollow microspheres are 4 times higher than BiOI nanosheets for degradation of RhB in 150&#xa0;min</td>
</tr>
<tr>
<td align="left">&#x2003;Bi<sub>12</sub>O<sub>17</sub>Br<sub>2</sub> nanotubes (<xref ref-type="bibr" rid="B37">Di et al., 2020</xref>)</td>
<td align="left">Solvothermal treatment</td>
<td align="left">300 Xe lamp</td>
<td align="left">Bi<sub>12</sub>O<sub>17</sub>Br<sub>2</sub> nanotubes, exhibiting 14.4 times higher activity than Bi<sub>12</sub>O<sub>17</sub>Br<sub>2</sub> nanoplates for CO<sub>2</sub> photoreduction</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>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 (<xref ref-type="fig" rid="F5">Figure 5B</xref>) (<xref ref-type="bibr" rid="B79">Jiang L. et al., 2012</xref>; <xref ref-type="bibr" rid="B98">Li L. et al., 2014</xref>; <xref ref-type="bibr" rid="B76">Jiang and Li, 2015</xref>) 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 (<xref ref-type="bibr" rid="B107">Lin et al., 2011</xref>; <xref ref-type="bibr" rid="B14">Cao J. et al., 2012</xref>; <xref ref-type="bibr" rid="B145">Peng et al., 2014</xref>). 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 (<xref ref-type="bibr" rid="B230">Yu et al., 2010</xref>). Wang et al. prepared p-type BiOBr and interfaced with n-type Bi<sub>2</sub>O<sub>2</sub>CO<sub>3</sub> by precipitation conversion. The photoactivity of BiOBr/Bi<sub>2</sub>O<sub>2</sub>CO<sub>3</sub> p-n junction is 14.8 folds that of bare Bi<sub>2</sub>O<sub>2</sub>CO<sub>3</sub> (<xref ref-type="bibr" rid="B183">Wang J. J. et al., 2020</xref>). Sun et al. prepared BiOBr/SnO<sub>2</sub> p-n heterojunctions to eliminate NO in visible light. Importantly, the charge transfer channels and directions at the BiOBr/SnO<sub>2</sub> interface were determined by theoretical calculations (<xref ref-type="fig" rid="F6">Figure 6B</xref>) and experiments (using XPS) (<xref ref-type="bibr" rid="B195">Wu et al., 2020</xref>). Similar research was extended to BiOCl and BiOI (<xref ref-type="table" rid="T1">Table 1</xref>).</p>
<p>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 (<xref ref-type="fig" rid="F5">Figure 5C</xref>). 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 (<xref ref-type="bibr" rid="B108">Lin et al., 2017</xref>) showed a 10% higher photoactivity than pristine BiOCl in elimination of RhB, which was due to the direct Z-scheme mechanism (<xref ref-type="fig" rid="F6">Figure 6C</xref>). In a new Z-scheme BiOBr/MnFe<sub>2</sub>O<sub>4</sub> nanocomposite, spontaneous transfer of photoelectron carriers contributed to the photoelectron-hole division and decelerated the electron-hole recombination (<xref ref-type="bibr" rid="B162">Sin et al., 2020</xref>). Other Z-scheme photocatalysts were also reported before (<xref ref-type="table" rid="T1">Table 1</xref>).</p>
</sec>
<sec id="s3-2">
<title>Elemental Doping</title>
<p>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., Fe<sup>3&#x2b;</sup>, Cu<sup>2&#x2b;</sup>, and Mn<sup>3&#x2b;</sup>) 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. Cu<sup>2&#x2b;</sup> was doped into BiOBr by using the solvothermal method to form the doping level (<xref ref-type="fig" rid="F7">Figure 7</xref>), which strengthened both light absorption and electron-hole isolation efficiency (<xref ref-type="bibr" rid="B124">Lv et al., 2020</xref>). Consequently, the Cu<sup>2&#x2b;</sup>-doped BiOBr showed a 2.28 times higher visible-light&#x2013;driven photocatalytic activity relative to pristine BiOBr. A similar method was used to prepare Fe<sup>2&#x2b;</sup>-doped BiOBr (<xref ref-type="bibr" rid="B103">Li W. et al., 2017</xref>). 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. (<xref ref-type="bibr" rid="B216">Yang W. et al., 2014</xref>). Other commonly used transitional metal dopants reported in BiOX include Zn<sup>2&#x2b;</sup> (<xref ref-type="bibr" rid="B102">Li J. et al., 2015</xref>; <xref ref-type="bibr" rid="B249">Zhou et al., 2019b</xref>), Ti<sup>4&#x2b;</sup> (<xref ref-type="bibr" rid="B77">Jiang G. et al., 2012</xref>), Al<sup>3&#x2b;</sup> (<xref ref-type="bibr" rid="B191">Weng et al., 2014a</xref>), Sn<sup>4&#x2b;</sup> (<xref ref-type="bibr" rid="B176">Tu et al., 2015</xref>), and Mn<sup>3&#x2b;</sup> (<xref ref-type="bibr" rid="B142">Pare et al., 2011</xref>).</p>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>Mechanistics of photocharge transport and surface transfer on BiOBr <bold>(A,D)</bold> and Cu-BiOBr <bold>(B,E)</bold> with norfloxacin and dissolved oxygen under full <bold>(A,B)</bold> arc and visible light <bold>(D,E)</bold> irradiation. The corresponding degradation kinetics under full arc <bold>(C)</bold> and visible light <bold>(F)</bold> (<xref ref-type="bibr" rid="B124">Lv et al., 2020</xref>). <bold>(G)</bold> Photocatalytic bacterial inactivation enhancement of B-BiOBr nanosheets (<xref ref-type="bibr" rid="B194">Wu et al., 2016</xref>). <bold>(H&#x2013;J)</bold> Organic degradation over La<sup>3&#x2b;</sup>-doped BiOBr and corresponded degradation kinetic for RhB and CIP (<xref ref-type="bibr" rid="B222">Yin et al., 2017</xref>).</p>
</caption>
<graphic xlink:href="fctls-02-839072-g007.tif"/>
</fig>
<p>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 (<xref ref-type="bibr" rid="B23">Chen et al., 2015</xref>). Many non-metals such as N, <xref ref-type="bibr" rid="B126">Fen-Qiang Ma et al. (2017)</xref>, <xref ref-type="bibr" rid="B244">Zhancheng Zhang et al. (2019)</xref>, <xref ref-type="bibr" rid="B138">Obeid et al. (2020)</xref>, <xref ref-type="bibr" rid="B115">Liu et al. (2021)</xref>, and <xref ref-type="bibr" rid="B120">L&#xf3;pez-Vel&#xe1;zquez et al. (2021)</xref> were doped into BiOX to improve the photocatalytic activity. Wang <italic>et al.</italic> prepared the boron-doped BiOBr nanosheets, in which the B dopants form an impurity level to accelerate charge separation (<xref ref-type="fig" rid="F7">Figure 7G</xref>) (<xref ref-type="bibr" rid="B194">Wu et al., 2016</xref>) Carbon doping can enhance the internal electric field of Bi<sub>3</sub>O<sub>4</sub>Cl and thereby increase bulk-charge separation to 80% (<xref ref-type="bibr" rid="B96">Li et al., 2015</xref>). This homogeneous carbon-doped Bi<sub>3</sub>O<sub>4</sub>Cl 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 <italic>et al.</italic> to prepare C-doped Bi<sub>24</sub>O<sub>31</sub>Cl<sub>10</sub> from oxytetracycline hydrochloride as a carbon and chlorine source (<xref ref-type="bibr" rid="B82">Jin et al., 2018</xref>).</p>
<p>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 La<sup>3&#x2b;</sup>-doped BiOBr microspheres produced by using an ionic liquid ([C16mim] Br)-assisted solvothermal route, (<xref ref-type="bibr" rid="B222">Yin et al., 2017</xref>), the substitution of Bi<sup>3&#x2b;</sup> by La<sup>3&#x2b;</sup> was monitored by XRD peak shift, while no La<sub>2</sub>O<sub>3</sub> 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 (<xref ref-type="fig" rid="F7">Figures 7H&#x2013;J</xref>). Similarly, Y-doped BiOCl improved the visible-light photocatalytic activity in tetracycline decomposition (<xref ref-type="bibr" rid="B248">Zhong et al., 2020</xref>). Moreover, europium and erbium were also used as dopants in BiOX recently (<xref ref-type="bibr" rid="B198">Xia et al., 2016</xref>).</p>
</sec>
<sec id="s3-3">
<title>Noble Metal Modification</title>
<p>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 (<xref ref-type="bibr" rid="B225">Yu et al., 2011</xref>; <xref ref-type="bibr" rid="B223">Yu C. L. et al., 2012</xref>). Li et al. prepared Pd/BiOBr by photodeposition (<xref ref-type="fig" rid="F8">Figure 8A</xref>) 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&#x2013;BiOBr interface. The coexistence of Pd and oxygen vacancies on BiOBr facilitates the adsorption of O<sub>2</sub> and toluene molecules (<xref ref-type="fig" rid="F8">Figure 8B</xref>). As a result, the Pd/BiOBr interface controls the charge division and activates O<sub>2</sub> and toluene, improving the photocatalytic activity of BiOBr by 1.5 times in 99% selective oxidation of toluene to benzaldehyde (<xref ref-type="fig" rid="F8">Figure 8C</xref>) (<xref ref-type="bibr" rid="B104">Li X. et al., 2020</xref>) Yu <italic>et al.</italic> investigated how noble metals (Rh, Pd, and Pt) deposition affected the photocatalytic behaviors of BiOX. The impact of the noble metals ranks as Pt &#x3e; Pd &#x3e; Rh under UV and as Rh &#x3e; Pt &#x3e; 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 (<xref ref-type="bibr" rid="B224">Yu et al., 2013</xref>).</p>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption>
<p>
<bold>(A)</bold> Schematic scheme for preparation of Pd/BiOBr; <bold>(B)</bold> photocatalytic selective toluene oxidation to benzaldehyde over Pd/BiOBr and <bold>(C)</bold> comparison of toluene conversion and selectivity among photocatalysts (reproduced with permission (<xref ref-type="bibr" rid="B104">Li X. et al., 2020</xref>)).</p>
</caption>
<graphic xlink:href="fctls-02-839072-g008.tif"/>
</fig>
</sec>
<sec id="s3-4">
<title>Interfacing with Carbon Materials</title>
<p>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 &#x3d; 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 <italic>via</italic> covalent bonds (<xref ref-type="fig" rid="F9">Figure 9A</xref>) (<xref ref-type="bibr" rid="B192">Weng et al., 2014b</xref>). Similarly, the BiOI/multi-walled carbon nanotube composites prepared by Xiong <italic>et al.</italic> using the solvothermal method photocatalytically outperformed pure BiOI owing to the interfacial charge-transfer (<xref ref-type="fig" rid="F9">Figure 9B</xref>) (<xref ref-type="bibr" rid="B167">Su et al., 2012</xref>). Graphene is another common carbon material to couple with BiOX. Li et al. prepared a BiOBr/graphene composite by an <italic>in situ</italic> solvothermal route using graphene oxide (<xref ref-type="fig" rid="F9">Figure 9C</xref>). The graphene oxide was reduced to graphene, and BiOBr NPs were formed on the surface. This composite has higher photocatalytic activity in degrading RhB (<xref ref-type="bibr" rid="B175">Tu et al., 2012</xref>). Reduced graphene oxide (RGO)/BiOCl hybrids were synthesized by Zhang et al. with graphene oxide as the precursor (<xref ref-type="bibr" rid="B106">Li Z. et al., 2017</xref>). 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 (<xref ref-type="fig" rid="F9">Figure 9D</xref>). Carbon quantum dots (CQDs) with quasi-spherical nanoparticles usually &#x3c;10&#xa0;nm in diameter have been introduced to BiOX recently. Li <italic>et al.</italic> prepared the CQD-modified BiOCl which showed the enhanced photocatalytic activity due to superior electron transfer ability of CQDs (<xref ref-type="bibr" rid="B41">Di et al., 2015</xref>). Furthermore, the nitrogen-doped CQD&#x2013;modified BiOBr was prepared by the same group to boost the photodegradation toward ciprofloxacin, rhodamine B, tetracycline hydrochloride, and bisphenol A (<xref ref-type="bibr" rid="B40">Di et al., 2016</xref>).</p>
<fig id="F9" position="float">
<label>FIGURE 9</label>
<caption>
<p>
<bold>(A)</bold> Mechanism of photocatalytic reaction over BiOX/CNT (<xref ref-type="bibr" rid="B192">Weng et al., 2014b</xref>). <bold>(B)</bold> Electron transfer between BiOI and MWCNT (<xref ref-type="bibr" rid="B167">Su et al., 2012</xref>). <bold>(C)</bold> Photodegradation over BiOBr/graphene (<xref ref-type="bibr" rid="B175">Tu et al., 2012</xref>). <bold>(D)</bold> Charge transfer of RGO/BiOCl photoanodes before and after phosphate modification (<xref ref-type="bibr" rid="B106">Li Z. et al., 2017</xref>) (all reproduced with permission).</p>
</caption>
<graphic xlink:href="fctls-02-839072-g009.tif"/>
</fig>
</sec>
<sec id="s3-5">
<title>Defect Engineering</title>
<p>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&#x2013;assisted solvothermal method and used it to fix atmospheric N<sub>2</sub> to NH<sub>3</sub> (<xref ref-type="fig" rid="F10">Figures 10A,B</xref>) (<xref ref-type="bibr" rid="B93">Li et al., 2015d</xref>). The sample without OV was also synthesized by further sintering in an O<sub>2</sub> atmosphere, and the color turned white (<xref ref-type="fig" rid="F10">Figure 10C</xref>). NH<sub>3</sub> was detected over BiOBr with OV, but not in BiOBr without OV (<xref ref-type="fig" rid="F10">Figure 10D</xref>). This was because the OV in BiOBr was the catalytic activation center and can chemisorb N<sub>2</sub> on the surface. Similarly, Xue et al. used BiOBr nanosheets with OV to realize N<sub>2</sub> to NH<sub>3</sub> (<xref ref-type="bibr" rid="B208">Xue et al., 2018</xref>). The Bi<sub>3</sub>O<sub>4</sub>Br 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 (<xref ref-type="bibr" rid="B38">Di et al., 2019</xref>). 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&#xa0;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 (<xref ref-type="bibr" rid="B186">Wang Q. et al., 2019</xref>). Cui et al. solvothermally prepared OV-rich BiOCl nanosheets (<xref ref-type="bibr" rid="B31">Cui et al., 2018</xref>). 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.</p>
<fig id="F10" position="float">
<label>FIGURE 10</label>
<caption>
<p>
<bold>(A)</bold> Schematic map of photocatalytic N<sub>2</sub> fixation over BiOBr with OV. <bold>(B)</bold> Photocatalytic N<sub>2</sub> fixation model with water as both the solvent and proton source. <bold>(C)</bold> Colors of BiOBr with or without OV. <bold>(D)</bold> Quantitative monitoring of NH<sub>3</sub> formed over different photocatalysts (<xref ref-type="bibr" rid="B93">Li et al., 2015d</xref>). <bold>(E)</bold> Illustration of the formation process of Bi<sub>24</sub>O<sub>31</sub>Br<sub>10</sub> with Bi-O vacancy pairs. Electrostatic potential of <bold>(F)</bold> Bi<sub>24</sub>O<sub>31</sub>Br<sub>10</sub> with Bi-O vacancy pairs and <bold>(G)</bold> perfect Bi<sub>24</sub>O<sub>31</sub>Br<sub>10</sub>. Electron localization function of <bold>(H)</bold> Bi<sub>24</sub>O<sub>31</sub>Br<sub>10</sub> with Bi-O vacancy pairs and <bold>(I)</bold> perfect Bi<sub>24</sub>O<sub>31</sub>Br<sub>10</sub> (<xref ref-type="bibr" rid="B36">Di et al., 2021</xref>).</p>
</caption>
<graphic xlink:href="fctls-02-839072-g010.tif"/>
</fig>
<p>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 (<xref ref-type="bibr" rid="B43">Di et al., 2018a</xref>). Liu and co-workers prepared the Bi<sub>24</sub>O<sub>31</sub>Br<sub>10</sub> atomic layer with &#x201c;Bi-O&#x201d; vacancy pairs by a mild polyvinylpyrrolidone (PVP) self-assembly strategy coupled with pH adjusting (see <xref ref-type="fig" rid="F10">Figure 10E</xref>). In contrast to the perfect surface, Bi<sub>24</sub>O<sub>31</sub>Br<sub>10</sub> with Bi-O vacancy pairs own large local electric field intensity (<xref ref-type="fig" rid="F10">Figures 10F,G</xref>). Furthermore, the presence of Bi-O vacancy pairs would create an electron delocalization hot spot (<xref ref-type="fig" rid="F10">Figures 10H,I</xref>), 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 (<xref ref-type="bibr" rid="B36">Di et al., 2021</xref>).</p>
</sec>
<sec id="s3-6">
<title>Facet Control</title>
<p>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<sup>&#x2b;</sup> 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) (<xref ref-type="fig" rid="F11">Figure 11A</xref>) (<xref ref-type="bibr" rid="B144">Peng et al., 2017</xref>). 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 <italic>et al.</italic> prepared the BiOCl with high ratios of [001] and (<xref ref-type="bibr" rid="B90">Li et al., 2012</xref>) facets (BiOCl-H1 and BiOCl-H2, respectively) under various acid conditions (<xref ref-type="fig" rid="F11">Figure 11D</xref>) (<xref ref-type="bibr" rid="B245">Zhao et al., 2020</xref>), which remarkably raised the RhB photodegradation efficiency. The apparent rate constant of BiOCl-H2 was 0.0961&#xa0;min<sup>&#x2212;1</sup>, about 2.7 times that of BiOCl-H1 (<xref ref-type="fig" rid="F11">Figures 11E,F</xref>). The Z-scheme facet heterojunction was constructed to accelerate charge separation and transportation (<xref ref-type="fig" rid="F11">Figure 11D</xref>). Zhang <italic>et al.</italic> 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 (<xref ref-type="bibr" rid="B78">Jiang J. et al., 2012</xref>).</p>
<fig id="F11" position="float">
<label>FIGURE 11</label>
<caption>
<p>
<bold>(A)</bold> Schematic map of the proposed formation mechanism of BiOBr-110. <bold>(B)</bold> RhB and <bold>(C)</bold> MO degradation over BiOBr-110 and BiOBr-001 (<xref ref-type="bibr" rid="B144">Peng et al., 2017</xref>). <bold>(D)</bold> Facet junction interface charge transportation. <bold>(E)</bold> Photodegradation of RhB and <bold>(F)</bold> dynamic fitting by using a first-order model (<xref ref-type="bibr" rid="B245">Zhao et al., 2020</xref>) (all reproduced with permission).</p>
</caption>
<graphic xlink:href="fctls-02-839072-g011.tif"/>
</fig>
</sec>
<sec id="s3-7">
<title>Thickness Tuning</title>
<p>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 (<xref ref-type="bibr" rid="B44">Di et al., 2018b</xref>; <xref ref-type="bibr" rid="B205">Xiong et al., 2018</xref>). The thickness-dependent photocatalytic activity toward salicylic acid degradation was reported by Li <italic>et al.</italic>, who prepared the thinner and thicker Bi<sub>3</sub>O<sub>4</sub>Cl through the liquid phase exfoliation under isopropanol or further recrystallization (<xref ref-type="bibr" rid="B94">Li J. et al., 2013</xref>). The thinnest Bi<sub>3</sub>O<sub>4</sub>Cl endows the highest photodegradation activity due to the highest internal electric field. The thinner thickness of Bi<sub>24</sub>O<sub>31</sub>Br<sub>10</sub> was prepared when a larger amount of NH<sub>4</sub>Br was used. The higher charge separation efficiency can be realized in thinner Bi<sub>24</sub>O<sub>31</sub>Br<sub>10</sub> nanosheets, thus leading to the formation of higher reactive oxygen species concentration, favoring the degradation of tetracycline hydrochloride (<xref ref-type="bibr" rid="B180">Wang C. Y. et al., 2017</xref>).</p>
</sec>
<sec id="s3-8">
<title>Morphology Control</title>
<p>The morphology control is a classic but effective strategy for boosting the photocatalytic activity of BIOX (<xref ref-type="bibr" rid="B52">Garg et al., 2018b</xref>; <xref ref-type="bibr" rid="B4">B&#xe1;rdos et al., 2019</xref>; <xref ref-type="bibr" rid="B5">B&#xe1;rdos et al., 2020</xref>). 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 (<xref ref-type="bibr" rid="B39">Di et al., 2014</xref>). 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 Bi<sub>12</sub>O<sub>17</sub>Br<sub>2</sub> nanotubes, exhibiting 14.4 times more activity than Bi<sub>12</sub>O<sub>17</sub>Br<sub>2</sub> nanoplates (<xref ref-type="bibr" rid="B37">Di et al., 2020</xref>). The enhanced activity is attributed to better CO<sub>2</sub> adsorption and activation, increased carrier separation, and CO desorption, which was induced by the surface tensile strain in Bi<sub>12</sub>O<sub>17</sub>Br<sub>2</sub> nanotubes.</p>
</sec>
<sec id="s3-9">
<title>Bismuth-Rich Strategy</title>
<p>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 (<xref ref-type="bibr" rid="B95">Li J. et al., 2017</xref>; <xref ref-type="bibr" rid="B189">Wang Z. et al., 2019</xref>). In addition, the bismuth-rich BiOX materials own more abundant tunable surface atomic configurations including surface atomic types, atomic quantity, and atomic distance. Bi<sub>24</sub>O<sub>31</sub>Br<sub>10</sub> materials display outstanding photocatalytic hydrogen evolution behavior, while the pristine BiOBr has been demonstrated to be inactive for photocatalytic hydrogen evolution (<xref ref-type="bibr" rid="B155">Shang et al., 2014</xref>).</p>
</sec>
</sec>
<sec id="s4">
<title>Purification of Pollutants and Photocatalyst Recovery</title>
<p>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<sup>&#x2212;</sup>). 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.</p>
<sec id="s4-1">
<title>Oxidation Degradation</title>
<p>Photooxidative degradation of many organic pollutants over modified BiOX has been extensively reviewed (<xref ref-type="bibr" rid="B217">Yang et al., 2018</xref>; <xref ref-type="bibr" rid="B156">Sharma K. et al., 2019</xref>; <xref ref-type="bibr" rid="B53">Garg et al., 2019</xref>). 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 (<xref ref-type="bibr" rid="B9">Brown and De Vito, 1993</xref>; <xref ref-type="bibr" rid="B22">Chen et al., 2010</xref>). Dyes even at extremely low levels (below 1&#xa0;ppm) are highly visible in water and severely worsen water environments (<xref ref-type="bibr" rid="B87">Ledakowicz and Gonera, 1999</xref>; <xref ref-type="bibr" rid="B55">Grzechulska and Morawski, 2002</xref>; <xref ref-type="bibr" rid="B34">Daneshvar et al., 2004</xref>). 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<sup>&#x2b;</sup>) 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 (<xref ref-type="bibr" rid="B81">Jiang et al., 2017</xref>). However, the RhB degradation by BiOBr/TiO<sub>2</sub> heterojunction was mediated by superoxide radical anions (O<sup>2&#x2212;</sup>), which was produced by single electron reduction of dissolved oxygen (<xref ref-type="bibr" rid="B215">Yang et al., 2021</xref>). Organic dye degradation was also investigated using different BiOX-based photocatalysts, namely, BiOCl/CeO<sub>2</sub> (<xref ref-type="bibr" rid="B243">Zhang Y. et al., 2020b</xref>), W-doped BiOCl (<xref ref-type="bibr" rid="B134">Mokhtari and Tahmasebi, 2021</xref>), Bi<sub>2</sub>WO<sub>6</sub>/BiOX (X &#x3d; Cl, Br, I) (<xref ref-type="bibr" rid="B35">Derikvand and Tahmasebi, 2021</xref>), and BiVO<sub>4</sub>/BiOX (X &#x3d; F, Cl, Br, I) (<xref ref-type="bibr" rid="B149">Razavi-Khosroshahi et al., 2019</xref>).</p>
<p>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 (<xref ref-type="bibr" rid="B8">Brain et al., 2004</xref>; <xref ref-type="bibr" rid="B111">Liu C. et al., 2012</xref>). 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 (<xref ref-type="bibr" rid="B152">Robinson et al., 2005</xref>). In general, the degradation of fluoroquinolones mainly involves amine side-chain degradative oxidation, defluorination, and decarboxylation (<xref ref-type="bibr" rid="B21">Chen and Chu, 2015</xref>). Of them, the degradation of the electron-rich amine side-chain to oxidized products is extremely important (<xref ref-type="bibr" rid="B165">Sturini et al., 2012</xref>). Different BiOX-based photocatalysts were also designed to reduce antibiotics. For example, Cu<sup>2&#x2b;</sup>-doped BiOBr (<xref ref-type="bibr" rid="B124">Lv et al., 2020</xref>), Nb<sup>5&#x2b;</sup> -doped BiOBr (<xref ref-type="bibr" rid="B190">Wei et al., 2020</xref>), and N-doped BiOCl (<xref ref-type="bibr" rid="B129">Maimaitizi et al., 2020</xref>) were used in the degradation of norfloxacin. Type II heterojunctions such as BiVO<sub>4</sub>/BiOCl (<xref ref-type="bibr" rid="B127">Ma X. et al., 2017</xref>), BiOBr/Fe<sub>2</sub>O<sub>3</sub> (<xref ref-type="bibr" rid="B56">Guo et al., 2017</xref>), and BiOBr/CdS (<xref ref-type="bibr" rid="B154">Senasu et al., 2021</xref>) can reportedly enhance the photodegradation of antibiotics.</p>
<p>Apart from the oxidation degradation of organic dyes and antibiotics, modified BiOX can also be applied to other common organics, including pharmaceutical active compounds (<xref ref-type="bibr" rid="B61">Heidari et al., 2020</xref>; <xref ref-type="bibr" rid="B50">Gao et al., 2021</xref>) and endocrine-disrupting chemicals (<xref ref-type="bibr" rid="B120">L&#xf3;pez-Vel&#xe1;zquez et al., 2021</xref>; <xref ref-type="bibr" rid="B196">Wu et al., 2021</xref>; <xref ref-type="bibr" rid="B233">Zhang H. et al., 2021</xref>). 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.</p>
</sec>
<sec id="s4-2">
<title>Reduction of Heavy Metals</title>
<p>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 (<xref ref-type="bibr" rid="B160">Shi et al., 1994</xref>; <xref ref-type="bibr" rid="B153">Salnikow and Zhitkovich, 2008</xref>). 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-Bi<sub>2</sub>S<sub>3</sub> heterojunctions <italic>via</italic> ion-exchange (<xref ref-type="bibr" rid="B119">Long et al., 2021</xref>). The performance of photo-reduced Cr(VI) was about 28.9 and 184.6 times higher than those of pure Bi<sub>2</sub>S<sub>3</sub> 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 CoFe<sub>2</sub>O<sub>4</sub>/BiOBr/graphene, (<xref ref-type="bibr" rid="B99">Li et al., 2019</xref>), BiOCl/Bi<sub>2</sub>S<sub>3</sub> (<xref ref-type="bibr" rid="B122">Lu et al., 2020</xref>), and BiOCl<sub>x</sub>Br<sub>1-x</sub> (<xref ref-type="bibr" rid="B71">Hussain et al., 2020</xref>). However, there is no example of using BiOX as photocatalysts into the reduction of other heavy metal ions.</p>
</sec>
<sec id="s4-3">
<title>Photocatalyst Recovery</title>
<p>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 <italic>et al.</italic> collected the Cu-doped BiOBr from suspension by centrifuge and then regenerated it by heating at 200&#xb0;C to remove the residual organic (<xref ref-type="bibr" rid="B124">Lv et al., 2020</xref>). 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 (<xref ref-type="bibr" rid="B172">Tettey et al., 2010</xref>; <xref ref-type="bibr" rid="B11">Cao C. Y. et al., 2012</xref>). A wide range of substrates have been employed for the immobilization of BiOX, such as activated carbon, ceramic fibers, and ceramic paper (<xref ref-type="bibr" rid="B210">Yadav et al., 2019</xref>; <xref ref-type="bibr" rid="B84">K&#xe1;sa et al., 2020</xref>; <xref ref-type="bibr" rid="B209">Yadav et al., 2020</xref>). The novel green BiOX (Cl, Br and I) was homogeneously immobilized on Al<sub>2</sub>O<sub>3</sub>-based ceramic fiber sheets, which exhibited an excellent photocatalytic performance and recyclability for MO, bisphenol A, and ampicillin disintegration under visible-light irradiation (<xref ref-type="bibr" rid="B210">Yadav et al., 2019</xref>).</p>
</sec>
</sec>
<sec id="s5">
<title>Summary and Prospects</title>
<p>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 &#x3d; Cl, Br, I) was reviewed and discussed to provide some guidance for future studies.</p>
<p>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.</p>
<p>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<italic>.</italic> 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.</p>
<p>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 <italic>in situ</italic> 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.</p>
<p>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.</p>
</sec>
</body>
<back>
<sec id="s6">
<title>Author Contributions</title>
<p>XL prepared and wrote the article, and FL and XH further edited the manuscript and checked the English writing.</p>
</sec>
<sec sec-type="COI-statement" id="s7">
<title>Conflict of Interest</title>
<p>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.</p>
</sec>
<sec sec-type="disclaimer" id="s8">
<title>Publisher&#x2019;s Note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors, and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
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