Fuyan
Kang‡
a,
Xiaona
Jiang‡
a,
Yao
Wang
a,
Juanna
Ren
bc,
Ben Bin
Xu
b,
Guoyang
Gao
a,
Zhanhua
Huang
*a and
Zhanhu
Guo
*b
aKey Laboratory of Bio-Based Material Science and Technology, Ministry of Education, Material Science and Engineering College, Northeast Forestry University, Harbin 150040, Heilongjiang, China. E-mail: huangzh1975@163.com
bMechanical and Construction Engineering, Faculty of Engineering and Environment, Northumbria University, Newcastle Upon Tyne, NE1 8ST, UK. E-mail: zhanhu.guo@northumbria.ac.uk
cCollege of Materials Science and Engineering, Taiyuan University of Science and Technology, Taiyuan, 030024, China
First published on 4th September 2023
Photocatalytic treatment of antibiotics in aqueous ecosystems has become a promising method. However, the low efficiency photogenerated charge separation and slow kinetics of the catalyst severely limit its deployment for industrial applications. Here, the three-dimensional bismuth tungstate (Bi2WO6)/bismuth oxyiodide (BiOI) loaded on biochar (BC/BWI) composite catalyst was designed for the efficient removal of tetracycline (adsorption capacity: 227.09 mg g−1, removal rate: 99.8%). Via construction of Z-scheme heterojunctions at the interface of Bi2WO6 and BiOI, the built-in electric field promotes the directional separation of photogenerated carriers to achieve efficient separation and utilization of photogenerated charges. Meanwhile, the introduction of electron-rich biochar (BC) effectively enhances the adsorption performance, photogenerated electron migration capacity and mass transfer process of the material. The introduction of BC and the building of Z-scheme heterojunctions effectively achieve the spatially synergistic separation of photogenerated charges. The ˙O2− dominates the photocatalytic process, according to the mechanistic studies. The degradation intermediate product testing revealed that tetracycline is efficiently degraded through two main pathways. This work provides ideas for the design of catalysts for the efficient removal of antibiotics from water bodies.
Among the reported many antibiotic and organic removal methods,11–13 photocatalysis has received widespread attention for its advantages of environmental protection, high efficiency and no secondary pollution.14–16 Bi2WO6 stands out in antibiotic removal with its excellent light absorption properties and suitable band gap structure.17 Many works have demonstrated the excellent performance of Bi2WO6 in the antibiotic removal process.18 Construction of heterojunction at the interface can effectively improve Bi2WO6 properties. Bi2WO6/BiOI exhibits excellent photocatalytic performance. Construction of heterojunction effectively separates photogenerated charges and reduces the recombination rate of photogenerated carriers.19 However, the photogenerated charge recombination rate still greatly limits the performance of the catalyst due to carrier recombination during the migration process.
Various biochars have been prepared and applied in energy storage, analysis and other fields.20–22 The electron-rich biochar can now significantly increase the reactive sites, improve adsorption performance, and accelerate photogenerated electron migration.23,24 These properties of biochar make it a suitable carrier for photocatalysts. To address the problems of low photogenerated charge separation and slow reaction kinetics, the construction of heterojunctions25 and the introduction of electron-rich biochar became the solution strategy.26
In order to achieve effective separation of photogenerated charges and increase the reaction kinetics, a space charge synergistic separation strategy was created. BC/BWI composites were prepared by the calcination method and solvothermal method. Photocatalytic removal of tetracycline shows excellent performance. The Z-scheme heterojunctions at the interface of Bi2WO6 and BiOI were constructed for the effective separation of photogenerated charges while the built-in electric field promoted the directional migration of photogenerated carriers. The introduction of electron-rich biochar effectively increases the active site and adsorption performance, accelerates the photogenerated electron migration and increases reaction kinetics. Synergistic charge separation of electron-rich carriers and Z-scheme heterojunctions increase the photocatalytic removal of tetracycline. Mechanistic studies indicated that ˙O2− is the main photoactive species. Analysis of reaction intermediates revealed that tetracycline is mineralized through two main degradation pathways. This research provides promising ideas for designing efficient antibiotic removal.
K = ln![]() | (1) |
qe = (C0 − Ct) × V/M | (2) |
![]() | (3) |
Detailed morphology and microstructure studies were conducted on the prepared samples using SEM and TEM. The SEM and TEM images of BC prepared by high-temperature carbonization and alkaline activation methods are shown in Fig. S1(a–f).† The TEM images demonstrate the 2D flat and thin layered structure of typical biomass carbon materials, which is also an important reason for the increase in specific surface area.27,28 As shown in Fig. 2a and Fig. S1(g–i),† Bi2WO6 is a flower like structure formed by crossing a large number of nanosheets. The pure BiOI is assembled from a large number of irregular nanosheets (Fig. 2b), which are loose, rough, and disordered. Fig. 2c shows a BCs/BWI0.2 composite catalyst well covered by Bi2WO6 and BiOI nanofragments. Unlike BC, it is clearly observed that these fragments are more loosely and loosely attached to BC.
To further demonstrate its details, Fig. 2c shows a large and distinct sheet-like structure in the lower part of the image, while the upper part is mostly composed of loose nano fragments with uncovered carbon voids. These findings demonstrated that the production of BiOI is an in situ growing process on Bi2WO6 nanoflowers, which can be regarded as a topological chemical conversion.29 Due to the abundant attachment points provided by carbon materials, the composite of the two aggregates on BCs forms the structure as shown in the figure. In theory, after adding KI and Na2WO6 solutions, BiOI is generated in the reaction system. As the reaction progresses, BiO+ is gradually released, and then BiO+ reacts with WO42− to generate Bi2WO6 based on the topological chemical reaction, which is in close contact with the continuously generated BiOI.30 As a result, a heterostructure was formed between Bi2WO6 and BiOI, enhancing charge separation in photocatalytic processes. With the increase of KI, Bi2WO6 nanoflower gradually collapses and decreases, and more and more BiOI is generated. The ideal molar ratio of Bi2WO6 to BiOI was therefore determined to be 20%, taking into account that stable heterostructures can show excellent photocatalytic performance.
Fig. 2d shows the TEM images of the BC/BWI0.2 composite catalyst, and Fig. 2(e and f) shows a locally enlarged view, both of which exhibit distinct spine-like structures. Fig. 2g shows the HR-TEM image of BC/BWI0.2. Not only can the carbon edge layer be clearly observed, but also three different sets of lattice stripes can also be clearly observed. The calculated lattice spacing is 0.82 nm and 0.29 nm, respectively. The presence of amorphous carbon layer will effectively promote the separation of photogenerated charges and also serve to enhance the stability of the catalyst.31 Among them, d = 0.82 nm corresponds to the (020) crystal planes of Bi2WO6. The d = 0.29 nm is in a better agreement with the (012) crystal planes of BiOI, which further proves the build of a clear heterojunction between Bi2WO6 and BiOI.32
The chemical composition and element content of BCs-BWI0.2 composite photocatalyst were analyzed by TEM EDS element mapping (Fig. 2(h–m)), and no other obvious impurities were found. From Fig. 2(i–m), the EDS spectrum of 50% BC/BWI0.2 shows strong signals of C, O, W, Bi, and I elements, with a uniform distribution, indicating a high purity of the composite catalyst.
The crystal structure of the BC/BWI was measured, as shown in Fig. 3a. The obvious diffraction peaks at 29.76°, 31.74°, 37.74°, 39.37°, 45.62°, 51.47°, 55.22°, 60.05°, 61.75°, 66.44°, 74.16°, and 75.36°, respectively, belong to the (012), (110), (112), (004), (020), (114), (122), (123), (006), (220), (320), and (130) crystal planes, which are in good agreement with the tetragonal BiOI (JCPDS no. 10-0445).33 These peaks are mostly sharp, and there are no other strong characteristic diffraction peaks, which proves that BiOI has a high purity and good crystallinity. Also, Bi2WO6 has a good match to the standard card (JCPDS no. 26-1044). In the BC/BWI of the composite catalyst, the diffraction peaks different from Bi2WO6, such as (112), (004), and (114), are characteristic diffraction peaks of BiOI with a good crystallinity. Although the peak intensity has decreased, it has not changed its unique crystal structure. More interestingly, as the BiOI content increases, the peak of Bi2WO6 shifts towards a lower angle (as shown by the red dashed line in the figure). This result effectively proves the doping of I− in the Bi2WO6 lattice and the successful in situ construction of BWI. The TEM images indicate the successful preparation of the composite catalyst.
The inherent structure and vibration changes of BC, BC/BW, and BC/BWI0.2 can be studied through Raman spectroscopy with a scanning range of 50–4000 cm−1, as shown in Fig. 3b. For BCs, the detected two typical peaks at 1344 cm−1 and 1574 cm−1, belong to the two broad peaks of the D-band and G-band of carbon materials.34 The largest element influencing the degree of carbon graphitization is the relative strength ratio of ID/IG. The lower the ID/IG value, the more graphitization there is. Compared to BC, BC/BW and BC/BWI0.2 show decreasing ID/IG values. As a result, high-temperature carbonization activation results in the graphitization of biochar, resulting in their transformation from disorder to order and the benign electron conduction in the composite system.
In addition, for BC/BW, the observed three typical peaks of 308, 796, and 830 cm−1, correspond to the Bi–W and O–W–O end antisymmetric/symmetric Ag modes of W–O tensile vibration and translational mode, respectively.35 For BC-BWI0.2, apart from the above peak positions, the observed only one peak located at 147 cm−1 is attributed to the Bi–I vibration of BiOI.36 These characterization analyses indicate that the synthesis of BC/BWI0.2 catalyst was successful, consistent with the XRD analysis.
The nitrogen adsorption measurement evaluated the specific surface area and pore structure properties. In Fig. 3c, a H3 hysteresis loop type IV with a P/P0 range of 0.8 to 1.0 is clearly visible in BC/BWI.37 As shown in Fig. 3d, all samples prepared in this study have a large number of micropores and mesoporous structures (pore size 0–2 nm). Table S1† shows the physical and chemical properties of materials. It can be seen that the specific surface area of composite BWI0.2 is only 64.45 m2·g−1. When BWI0.2 is loaded onto BC, the surface area is significantly increased to 1759.99 m2·g−1. As the content of BiOI increases, the specific surface area increases, with BC/BWI0.1, BC/BWI0.2, BC/BWI0.3, and BC/BWI0.4 being 1215.98, 1759.99, 1962.42, and 2358.99 m2·g−1, respectively, higher than BC/BW (869.41 m2·g−1). This means that after partially dense Bi2WO6 is replaced by loose BiOI, the specific surface area of the composite continues to increase. The larger specific surface area is conducive to carrier migration and provides more active site for the composite catalyst.
Furthermore, more-small sized BiOI fragments enter the pore structure of BC, resulting in a smaller pore size. During the growth process, the composite enters the pores, cross aggregates, and accumulates on the surface of carbon materials, which may be the reason for the increase in pore volume. This will be beneficial for providing more adsorption centers and improving the catalytic performance of the complex.
The UV-Vis diffuse reflectance spectra were tested to examine the series of optical properties of photocatalysts, as shown in Fig. 3e. In the above experiment, the absorption edge of pure Bi2WO6 was at 440 nm. In Fig. 3e, the light absorption edge of BiOI is about 670 nm, and its absorption ability at wavelengths of 200–800 nm is superior to other samples. Thus the visible light absorption edge was significantly widened by utilizing the special heterojunction structure of the two. The visible light absorption edge of the composite catalyst BC/BWI0.2 is about 630 nm, indicating a red shift on the basis of BC/BW, which is conducive to the absorption and utilization of visible light by the photocatalyst. The variation curve of BiOI is shown in Fig. 3f, where BiOI is an indirect transition with n = 1. Therefore, the bandgap of BiOI is 2.02 eV, similar to the reported value in the literature.38,39 The bandgap of Bi2WO6 is 2.91 eV, as shown in Fig. 3f. The band gap mainly reflects the characteristics of semiconductors. Low band gaps can promote a relatively low electron excitation energy, and more conductive band electrons can be used for photocatalysis.
The chemical state and surface element composition of BC/BWI0.2 composites were studied by XPS, and the results are shown in Fig. 4. As shown in Fig. 4a, only Bi, I, C, W and O elements were found in the of BC/BWI0.2 composite material. The peak of C 1s at 284.6 eV can be assigned as the carbon signal used for calibration in the instrument.40,41 In the spectrum of Bi 4f, as shown in Fig. 4b, the two peaks with binding energies around 163.93 eV and 158.65 eV, in the trivalent oxidation state, correspond to the bimodal signals of Bi 4f5/2 and Bi 4f7/2.42,43Fig. 4c shows the signal peak of the oxygen element. The binding energy at 529.46 eV and 530.79 eV corresponds to the W–O bond in Bi2WO6 and the Bi–O bond in Bi2O2 layered structure respectively. The binding energy at 532.31 eV can be attributed to the O2− anion in BWI0.2.44 The peaks located at 36.96 eV and 34.83 eV correspond to W 4f5/2 and W 4f7/2, respectively, and can be divided into W6+ oxidation states in the Fig. 4b.
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Fig. 4 (a) XPS full-spectra of 50% BC/BWI0.2, XPS high-resolution spectra of (b) Bi 4f, (c) O 1s, (d) W 4f, (e) I 3d and (f) C 1s. |
The existence of Bi2WO6 and BiOI in the catalyst is further supported by the XPS spectrum. It can be seen from Fig. 4e that on the I 3d orbital, a splitting peak appears at the binding energy of about 629.96 eV and 618.48 eV, which belongs to I 3d3/2 orbital and I 3d5/2 orbital respectively, confirming the valence state of I−1 in the sample.45 The above results confirm the successful recombination of Bi2WO6 and BiOI and the possibility of forming heterojunctions, which is consistent with the literature description.39
The photocatalytic efficiency mainly depends on the recombination rate of photogenerated charge, as photoluminescence is caused by the recombination of charge carriers. According to Fig. 5a, the strongest absorption peak of the composite catalyst is at 378 nm. Under the same experimental conditions, the emission intensity of BC/BWI0.2 is the lowest, indicating that the introduction of BiOI can significantly promote the separation of photo induced carriers, which can be attributed to the interface electric field.46 Among them, the emission intensity of BC/BWI0.2 is the lowest, significantly improving the separation rate of photo excited carriers. It has been proven that the activity of the BC/BWI0.2 catalyst is the strongest.
Fig. 5b shows the EIS Nyquist plot of the prepared sample. The smaller the arc radius in the figure, the higher the carrier transport efficiency in the catalyst.47 The arc radius of BC/BWI0.2 is significantly smaller than that of other samples, supporting the higher photo generated electron and hole separation rate of this composite material. The experimental results are consistent with PL, so it can be predicted that BC/BWI0.2 sample may exhibit a higher photocatalytic activity.
Furthermore, the charge separation of the catalyst was characterized using a transient photocurrent response, as shown in Fig. 5c. Under light excitation, an extremely significant photocurrent was generated instantly, and the photocurrent density of BC/BWI for several consecutive cycles was higher than that of other samples. Among them, the photocurrent density of BC/BWI0.2 is about 300 times that of the original Bi2WO6 and 4.5 times that of BC/BW. It has been proven that the electric field between BiOI and Bi2WO6 is conducive to the separation and transfer of photogenerated charge.
The LSV data demonstrates that BC/BWI has a minimum overpotential, which indicates that BC/BWI can effectively separate photogenerated charges (Fig. 5d). The Mott Schottky method was used to measure the flat band (FB) potential of the catalyst, and Fig. 5(e and f) shows the Mott Schottky plot of BiOI and Bi2WO6 measured at voltage frequencies of 500, 800 and 1000 Hz. Calculate EFB using the x-axis intercept of the linear part of the curve and convert the result into NHE potential. The slope of the Mott Schottky curve indicates that BiOI and Bi2WO6 are p-type and n-type semiconductors, respectively.48 Therefore, the EFB of BiOI and Bi2WO6 are 1.35 eV and −0.25 eV (vs. NHE, pH = 7). The above electrochemical analysis well confirms that the introduction of BiOI promotes the improvement of charge separation rate in Bi2WO6, among which the BC/BWI0.2 sample is expected to demonstrate the most excellent photocatalytic performance.
The photocatalytic degradation performance of 50 mg L−1 TC (100 mL) was evaluated through the photocatalytic degradation experiments, and all samples reached adsorption desorption equilibrium after 40 minutes. The experimental data of TC degradation at 420 nm is shown in Fig. 7a. The degradation rate of pure Bi2WO6 is about 27.53% within 1 hour, and the degradation rate of pure BiOI is about 17.73% within 1 hour. In addition, we also tested that the degradation efficiency of BWI0.2 on TC was about 51.84%, which is 1.5 times that of Bi2WO6 and nearly 3 times that of BiOI. However, it is evident in the figure that the adsorption capacity of Bi2WO6, BiOI, and BWI0.2 is almost zero. With the increase of BC, the adsorption capacity of the composite catalyst for TC is greatly improved. At the same time, the photocatalytic efficiency has also slightly improved, thanks to the fact that BC can serve as receptors for electron migration. The removal rate of TC by BC/BWI0.2 is as high as 99.84%, and the removal rate of TC by 50% BC/BW is about 76.05%, further proving that the entry of BiOI can form heterojunctions with Bi2WO6 to promote photocatalytic activity. The removal rates of TC by Bi2WO6, BiOI, BWI0.2, BC/BW, BC/BWI0.1, BC/BWI0.2, BC/BWI0.3, and BC/BWI0.1 were 37.08%, 17.73%, 51.84%, 96.24%, 99.77%, 93.44%, and 90.03%, respectively. According to Fig. 7b, the slopes of the pseudo first order kinetic equation curves k corresponding to the photocatalyst are 6.73, respectively ×10−3, 2.82 × 10−3, 1.28 × 10−2, 8.16 × 10−2, 3.99 × 10−2, 8.66 × 10−2, 3.07 × 10−2 and 2.90 × 10−2 min−1. The obvious BCs/BWI0.2 has better photocatalytic activity, which is consistent with the above characterization results. This work was thoroughly compared with other work (Table S4†). This study shows a significant advantage in the removal of TC, which also proves the efficiency of the space charge synergistic separation.
Stability and repeatability are important evaluation criteria for the practical application of photocatalysts. The cyclic test results in Fig. 7c and d show that the degradation efficiency of BC/BWI0.2 has hardly decreased after 5 cycles on TC, which can be applied to practical wastewater treatment fields. On this basis, scavenger experiments were conducted in order to investigate the role of photoactive species. Ammonium oxalate (AOM), dimethyl sulfoxide (DMSO), p-benzoquinone (BQ) and isopropanol (IPA) are used as h+, e−, ˙O2− and ˙OH scavenger respectively. Compared with the blank group, the degradation effect of the experimental group with the addition of trapping agent was reduced to different degrees. The rate constant decreases most significantly with the addition of BQ (k = 9.31 × 10−3 min−1). This indicates that ˙O2− play a dominant role in the photocatalytic degradation of TC.
ESR testing determined the role of active components in the reaction system through DMPO-˙O2−, DMPO-˙OH, TEMPO-h+, and TEMPO-e−. In the absence of light in Fig. 8(a) and (b), no ESR signal was observed. When BC/BWI0.2 and DMPO were mixed under light for 5 and 10 minutes, the characteristic peaks of ˙O2− and ˙OH both responded and gradually increased. This indicates that in the catalytic system, ˙O2− and ˙OH were generated under light conditions. As the illumination time increases, the signal intensity of ˙O2− increases more significantly, which is consistent with the results of free radical capture experiments. As shown in Fig. 8(c) and (d), compared to dark conditions, the signal intensity of e− and h+ decreased significantly within 5–10 minutes under light conditions, indicating the continuous generation of h+ and e− during the photocatalytic reaction process.
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Fig. 8 ESR spectrum of (a) DMPO-˙O2−; (b) DMPO-˙OH; (c) TEMPO-h+ and (d) TEMPO-e− under both the dark and visible light irradiation. |
To further understand the degradation process, the TC degradation intermediates were determined by LC-MS. Based on the relevant data (Fig. S2†), we propose two possible degradation pathways. Under light irradiation, BC/BWI produces the strongly oxidizing ˙OH. In pathway I, first, ˙OH attacks the hydroxyl functional group on the molecule, followed by an oxidation reaction to produce P1 (m/z = 475). Subsequently, the photoactive species generate P2 (m/z = 388) by attacking the ketone and hydroxyl groups on P1. P2 as an unstable intermediate loses its hydroxyl group to further produce P3 (m/z = 318), P4 (m/z = 242) and P5 (m/z = 165).54 These products then undergo further mineralization reactions to produce H2O and CO2. In the degradation pathway II, h attacks the benzene ring in TC and introduces hydroxyl and ketone groups to produce P6 (m/z = 459). P6 loses N-methyl and further produces P7 (m/z = 415). P7 undergoes a series of reactions such as carbon ring cleavage and loss of hydroxyl group to produce P8 (m/z = 344). P8 undergoes decarboxylation to produce P9 (m/z = 300). P9 undergoes reactions such as dehydroxylation and dealkalization to produce subsequent reaction products (P10, m/z = 246). On this basis, the intermediate products undergo oxidative decomposition and ring opening reactions to produce small molecule products (H2O, CO2 and NH4+).55,56 TC is mineralized through both of these pathways to produce small molecule products (Fig. 9).
With these data (Fig. 7 and 8), the generation process of photoactive species is proposed. Under visible light irradiation, the semiconductor undergoes an energy band jump (eqn (4) and (5)). e− and h+ are produced on the band gap structure of the semiconductor, respectively. Based on the photoelectric characterization data (Fig. 3e, f and 5e, f), Bi2WO6 and BiOI band gap structures are calculated (ECB1 = −0.15 eV and EVB1 = 2.59 eV; ECB2 = −0.42 eV and EVB2 = 1.45 eV). In this case, two heterojunctions may be formed at the semiconductor interface (type II heterojunction and Z-scheme heterojunction).57 In the type II heterojunction case, the conduction band (ECB2) electrons of BiOI will migrate to the conduction band (ECB1) of Bi2WO6. Meanwhile, the holes in the valence band (EVB1) of Bi2WO6 will migrate to the valence band (EVB2) of BiOI. The value (ECB1 = −0.15 eV) of ECB1 is less than the generation potential of ˙O2− (Eθ = −0.33 eV). The value (EVB2 = +1.45 eV) of EVB1 is also greater than the generation potential of OH−/˙OH (Eθ = +1.99 eV) and H2O/˙OH (Eθ = +2.38 eV). The formation of type II heterojunction at the interface is unable to form ˙O2− and ˙OH in the photocatalytic process, which is not consistent with the experimental reality (Fig. 7e and 8).
Bi2WO6 + hv → ECB1(e−) + EVB1(h+) | (4) |
BiOI + hv → ECB2(e−) + EVB2(h+) | (5) |
ECB1(e−) → EVB2(h+) | (6) |
ECB2(e−) → BC | (7) |
e− + O2 → ˙O2− | (8) |
˙O2− + H+ + e− → ˙OH + OH− | (9) |
OH− + h+ → ˙OH | (10) |
˙OH + TC → degradation products | (11) |
˙O2− + TC → degradation products | (12) |
h+ + TC → degradation products | (13) |
The formation of type II heterojunction is inconsistent with the experimental situation, which indicates that the formation of Z-scheme heterojunction. ECB1 electrons leap to EVB2 with holes complex (eqn (6)). The photogenerated electrons on ECB2 also efficiently migrate to BC. Meanwhile, EVB1 and ECB2 generate photoactive radicals with environmental factors (H2O and O2), respectively (eqn (7)–(13)). The formation of Z-scheme heterojunction effectively separates the photogenerated charge and also preserves the redox ability of the material.58 BC acts as an electron-rich carrier to accelerate the migration of photogenerated electrons and further enhance photocatalytic performance.59–63 This work introduces electron-rich carriers and constructs Z-scheme heterojunction is to achieve efficient removal of TC. Charge synergistic separation strategy is a favorable idea for designing efficient photocatalysts (Fig. 10).
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Fig. 10 Possible path and photocatalytic mechanism of photocatalytic TC degradation by BC/BWI under solar radiation. |
Based on the above data, the TC removal mechanism is proposed. Under visible light irradiation, the semiconductor material undergoes an energy band jump to produce e− and h+. Z-scheme heterojunction is formed at the interface of Bi2WO6 and BiOI. Because the two semiconductor types are different, there is a built-in electric field at the interface. The presence of the built-in electric field promotes the directional migration of photogenerated carriers and accelerates the separation of photogenerated charges. Meanwhile, the introduction of the electron-rich carrier BC increases the adsorption sites of the material and accelerates the mass transfer process of TC. On this basis, BC also effectively promotes the migration of photogenerated electrons and reduces the complex rate of photogenerated charges. Efficient separated photogenerated carriers are involved in the generation of photoactive species. Photoactive species were involved in the degradation of TC, which was generated into small molecule products through two main pathways.
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3qi01283b |
‡ These authors contributed equally. |
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