Yuze 
            Wu
          
        
      a, 
      
        
          
            Jingchao 
            Liu
          
        
       b, 
      
        
          
            Jinxia 
            Zhao
          
        
      a, 
      
        
          
            Chunhong 
            Jin
          
        
      a, 
      
        
          
            Hailong 
            Ren
          
        
      a, 
      
        
          
            Yilin 
            Yin
          
        
      *a and 
      
        
          
            Zenghe 
            Li
b, 
      
        
          
            Jinxia 
            Zhao
          
        
      a, 
      
        
          
            Chunhong 
            Jin
          
        
      a, 
      
        
          
            Hailong 
            Ren
          
        
      a, 
      
        
          
            Yilin 
            Yin
          
        
      *a and 
      
        
          
            Zenghe 
            Li
          
        
       *a
*a
      
aBeijing University of Chemical Technology, Beijing 100029, China. E-mail: lizh@mail.buct.edu.cn; yinyilin361@163.com
      
bSchool of Computer Science and Engineering, Beihang University, Beijing 100191, China. E-mail: jingchaoliu1992@163.com
    
First published on 13th April 2024
A BiO2−x/COF composite was successfully synthesized by simple mechanical ball milling. Compared to pure BiO2−x and COFs, the BiO2−x/COF composite (1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9) showed superior photocatalytic capability. Under visible light irradiation for 90 min, the photocatalytic degradation rate of DCF reached 97%. In addition, the characterization results showed that the formation of heterojunctions and the increase in oxygen vacancy concentration were the reasons for the enhancement of the photocatalytic activity. It is confirmed by free radical capture experiments that ˙O2− and h+ are the main reactive substances in the photocatalytic process. The photocatalytic degradation mechanism of the composite and the photocatalytic degradation pathway of diclofenac were deduced.
9) showed superior photocatalytic capability. Under visible light irradiation for 90 min, the photocatalytic degradation rate of DCF reached 97%. In addition, the characterization results showed that the formation of heterojunctions and the increase in oxygen vacancy concentration were the reasons for the enhancement of the photocatalytic activity. It is confirmed by free radical capture experiments that ˙O2− and h+ are the main reactive substances in the photocatalytic process. The photocatalytic degradation mechanism of the composite and the photocatalytic degradation pathway of diclofenac were deduced.
Not long ago, BiO2−x was reported to have a narrower band gap and a favorable response to visible light, even extending up to 850 nm, which requires only a simple one-step hydrothermal method to synthesise semiconductor catalysts rich in oxygen vacancies.8–10 Taking these advantages into account, BiO2−x is being researched as a highly effective photocatalyst for degrading pollutants and inactivating bacteria when exposed to visible light.11,12 However, due to its narrow band gap, it is easier to recombine photogenerated electron–holes. Some scholars have also utilized bismuth-containing semiconductor materials to enhance the recombination of photocatalytic carriers by constructing heterojunctions, thereby improving the photocatalytic efficiency and offering a novel approach to the modification of BiO2−x.13–16 Therefore, many studies have modified BiO2−x to improve its photocatalytic activity.17–19 It has been reported that the photocatalytic activity of BiO2−x can be further improved by adjusting the thickness and Ni doping.10,20 Chen et al. used N-doped GQDs to modify BiO2−x to enhance its response to the full spectrum.21 The photocatalytic performance can also be improved by forming heterojunctions to inhibit the recombination of electron–hole pairs. For example, Jia et al.22 prepared (BiO)2CO3/BiO2−x/graphene photocatalysts and Liu et al.23 constructed Z-scheme BiO2−x/BiOBr photocatalysts; both materials exhibited higher photocatalytic activity and stability, which can be attributed to the improved efficiency of charge separation and transfer.
COFs have good application prospects in the degradation of pollutants because of their open and designable structure.24–27 Many 2D COFs have graphene-like π–π conjugate structures, and the existence of delocalized π bonds enables the COF to have a high carrier transport speed in the stacking direction, which is extremely beneficial for the photocatalytic reaction. They feature adjustable voids, large conjugated structures conducive to electron transfer, and strong absorption of visible light. They are often combined with other semiconductor photocatalysts to increase the specific surface area, enhance visible light absorption, and promote electron transfer. Zhang et al.28 modified 2D BiOBr and 2D TzDa covalent organic frameworks (COFs) by the hydrothermal method and designed an efficient Z-type heterojunction photocatalyst, which is of great significance for solar energy wastewater purification. Based on this property, COFs are commonly used in combination with other semiconductor photocatalysts to enhance their specific surface area, improve visible light absorption, and facilitate electron transfer.29–31 Therefore, in this study, we synthesized a BiO2−x/COF composite material. Taking diclofenac as an example, the photocatalytic degradation performance and stability of the composite were evaluated. Photocatalytic carriers were further investigated and the band structure was calculated. The mechanism of enhancement of BiO2−x/COF photocatalytic activity and the degradation pathway of diclofenac are discussed.
![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9.5BiO2−x, 1COF
9.5BiO2−x, 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x, 1.5COF
9BiO2−x, 1.5COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 8.5BiO2−x, and 2COF
8.5BiO2−x, and 2COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 8BiO2−x.
8BiO2−x.
          ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 2‰ acetic acid aqueous solution = 80
2‰ acetic acid aqueous solution = 80![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 20, flow rate 1.0 mL min−1, and sample size 20 μL. The product of the DCF degradation pathway was detected using LC-MS (UPLC/Premier); a triple quadrupole detector equipped with an electrospray ionization (ESI) source was utilized for analysis. The scan range was extended from m/z 50 to 400. Methanol/0.1% formic acid aqueous solution (80/20) was selected as the mobile phase.
20, flow rate 1.0 mL min−1, and sample size 20 μL. The product of the DCF degradation pathway was detected using LC-MS (UPLC/Premier); a triple quadrupole detector equipped with an electrospray ionization (ESI) source was utilized for analysis. The scan range was extended from m/z 50 to 400. Methanol/0.1% formic acid aqueous solution (80/20) was selected as the mobile phase.
      
    
    
      
      ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 1 and the peak of the COF was obtained, which successfully confirmed the conjecture. Fig. 1b shows the FTIR spectra of the COF, BiO2−x and 1COF
1 and the peak of the COF was obtained, which successfully confirmed the conjecture. Fig. 1b shows the FTIR spectra of the COF, BiO2−x and 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x, which were used to determine the chemical composition of 1COF
9BiO2−x, which were used to determine the chemical composition of 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x. The positions of the characteristic peaks of the composite were consistent with those of the COF and BiO2−x, wherein 1621 cm−1 comes from the stretching vibration of the imine bond of the COF,32 and 592 cm−1 and 533 cm−1 correspond to the Bi–O bond vibration characteristic peaks of BiO2−x,33,34 In comparison, BiO2−x and the COF can be identified in the BiO2−x/COF composites. With the increase of COF content, the absorption band strength of the COF gradually increases, while that of BiO2−x relatively decreases, further demonstrating the coexistence of the two contents of BiO2−x and the COF in the composite materials.
9BiO2−x. The positions of the characteristic peaks of the composite were consistent with those of the COF and BiO2−x, wherein 1621 cm−1 comes from the stretching vibration of the imine bond of the COF,32 and 592 cm−1 and 533 cm−1 correspond to the Bi–O bond vibration characteristic peaks of BiO2−x,33,34 In comparison, BiO2−x and the COF can be identified in the BiO2−x/COF composites. With the increase of COF content, the absorption band strength of the COF gradually increases, while that of BiO2−x relatively decreases, further demonstrating the coexistence of the two contents of BiO2−x and the COF in the composite materials.
      |  | ||
| Fig. 1 (a) XRD patterns of BiO2−x combined with COFs of different weights; (b) Infrared images of BiO2−x combined with COF of different weight. | ||
        Fig. 2(a) shows the scanning electron microscopy image of BiO2−x, and it can be seen that the synthesized BiO2−x has a small fragment morphology.35Fig. 2(b) shows the SEM image of the COF,32 and it can be clearly seen that the COF is a sheet material. As shown in Fig. 2(c), BiO2−x is uniformly dispersed on the surface of the COF, and from the mapping images in Fig. 2(g), (h), (i) and (j), the Bi, O, N and C elements of 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x are uniformly distributed. This indicates that BiO2−x and the flake structure of the COF are tightly bound in the composite material. Fig. 2(d) shows the TEM image of 1COF
9BiO2−x are uniformly distributed. This indicates that BiO2−x and the flake structure of the COF are tightly bound in the composite material. Fig. 2(d) shows the TEM image of 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x. It clearly shows the tight attachment of BiO2−x small fragments to the surface of COF nanosheets, indicating the formation of a well-defined heterojunction between BiO2−x and the COF. The HRTEM images are presented in Fig. 2(e) and (f) for the 1COF
9BiO2−x. It clearly shows the tight attachment of BiO2−x small fragments to the surface of COF nanosheets, indicating the formation of a well-defined heterojunction between BiO2−x and the COF. The HRTEM images are presented in Fig. 2(e) and (f) for the 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x composite material. The crystal plane (110) of the COF can be clearly seen in the 20 nm scale, corresponding to a lattice spacing of 2.240 nm; this result further shows that the reason why the composites do not show the diffraction peak of the COF in XRD is that the COF content is less. Fig. 2(e) shows a local magnification of Fig. 2(f), and it can be clearly observed that lattice fringe spacing of 0.320 and 0.282 nm corresponds to the (111) and (200) lattice planes of BiO2−x, respectively.22,36 The HRTEM images provided further evidence of the coexistence of BiO2−x and the COF, as well as the formation of an interfacial heterojunction. Through the above characterization, it is further concluded that the two semiconductors are closely combined.
9BiO2−x composite material. The crystal plane (110) of the COF can be clearly seen in the 20 nm scale, corresponding to a lattice spacing of 2.240 nm; this result further shows that the reason why the composites do not show the diffraction peak of the COF in XRD is that the COF content is less. Fig. 2(e) shows a local magnification of Fig. 2(f), and it can be clearly observed that lattice fringe spacing of 0.320 and 0.282 nm corresponds to the (111) and (200) lattice planes of BiO2−x, respectively.22,36 The HRTEM images provided further evidence of the coexistence of BiO2−x and the COF, as well as the formation of an interfacial heterojunction. Through the above characterization, it is further concluded that the two semiconductors are closely combined.
|  | ||
| Fig. 2  SEM images of (a) BiO2−x, (b) COF, and (c) 1COF ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) : ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x; (d) TEM image of the 1COF ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) : ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x sample; (e and f) HRTEM image of 1COF ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) : ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x; and (g)–(j) mapping images of 1COF ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) : ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x. | ||
The surface compositions and chemical states of pure BiO2−x, COF and 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x samples were analyzed by XPS. Fig. 3(a) shows the XPS survey spectra of BiO2−x, the COF, and 1COF
9BiO2−x samples were analyzed by XPS. Fig. 3(a) shows the XPS survey spectra of BiO2−x, the COF, and 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x. Compared with pure BiO2−x and the COF, four elements C, N, O and Bi can be observed in the composite material, and no other impurity elements can be observed in the spectrum. Fig. 3(b) shows the XPS spectral comparison of the O1s peaks of BiO2−x, the COF and 1COF
9BiO2−x. Compared with pure BiO2−x and the COF, four elements C, N, O and Bi can be observed in the composite material, and no other impurity elements can be observed in the spectrum. Fig. 3(b) shows the XPS spectral comparison of the O1s peaks of BiO2−x, the COF and 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x. It can be seen from the figure that the positions of the peaks of the composite material change relative to pure BiO2−x and the COF. First, the C 1s spectrum was analyzed. In the spectrum, the peaks at 284.8 eV, 285.6 eV, and 288.6 eV correspond to C
9BiO2−x. It can be seen from the figure that the positions of the peaks of the composite material change relative to pure BiO2−x and the COF. First, the C 1s spectrum was analyzed. In the spectrum, the peaks at 284.8 eV, 285.6 eV, and 288.6 eV correspond to C![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif) C, C
C, C![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif) N, and C
N, and C![[double bond, length as m-dash]](https://www.rsc.org/images/entities/char_e001.gif) O functionalities, respectively (Fig. S2†). There are three O 1s peaks at 529.7 eV, 531.2 eV and 532.5 eV,10,37,38 which can be assigned to the lattice oxygen, surface oxygen vacancies and surface adsorbed oxygen, respectively. Fig. 3(c) shows the Bi 4f spectrum of the composite material that has two peaks at 164.5/163.8 eV and 159.1/158.5 eV, which were attributed to Bi 4f7/2 and Bi 4f5/2, respectively. Compared with pure BiO2−x, the XPS peak of Bi 4f shifted to higher binding energy. Fig. 3(d) shows the N 1s spectrum of the composite material that has a peak at 399.1 eV, which moves toward the lower binding energy relative to the binding energy of the N 1s spectrum in the COF, indicating that there is electron transfer at the interface of the two materials, electrons move from high binding energy to low binding energy, and electrons move from the BiO2−x surface to the COF surface. The two materials are highly bonded.
O functionalities, respectively (Fig. S2†). There are three O 1s peaks at 529.7 eV, 531.2 eV and 532.5 eV,10,37,38 which can be assigned to the lattice oxygen, surface oxygen vacancies and surface adsorbed oxygen, respectively. Fig. 3(c) shows the Bi 4f spectrum of the composite material that has two peaks at 164.5/163.8 eV and 159.1/158.5 eV, which were attributed to Bi 4f7/2 and Bi 4f5/2, respectively. Compared with pure BiO2−x, the XPS peak of Bi 4f shifted to higher binding energy. Fig. 3(d) shows the N 1s spectrum of the composite material that has a peak at 399.1 eV, which moves toward the lower binding energy relative to the binding energy of the N 1s spectrum in the COF, indicating that there is electron transfer at the interface of the two materials, electrons move from high binding energy to low binding energy, and electrons move from the BiO2−x surface to the COF surface. The two materials are highly bonded.
|  | ||
| Fig. 3  XPS spectra of BiO2−x, the COF and 1COF ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) : ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x: (a) survey, (b) O 1s, (c) Bi 4f, and (d) N 1s. | ||
To further analyse the oxygen vacancies in the catalyst, the EPR test was conducted on BiO2−x, the COF and the 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x composite. As shown in Fig. 4(a), it can be seen that BiO2−x has a large and wide peak with g = 2.05.10,37–39 This is attributed to bismuth defects caused by oxygen vacancies in the photocatalytic material. The EPR signal becomes stronger after compositing, indicating that the oxygen vacancy concentration increases after compositing, which is also conducive to the improvement of photocatalytic degradation performance. The embedded figure is a comparison between the enlarged yellow region of the composite material and the EPR of the COF. It can be clearly seen from the figure that the COF can detect vibration signals at g = 2.003, indicating that the COF also has oxygen vacancies,40 and the EPR signal of the composite has a wide peak of bismuth defects caused by oxygen vacancies at g = 2.05. There is also an oxygen vacancy peak of g = 2.004. It is further proved that the composite material has oxygen vacancies. This conclusion is consistent with the previous XPS spectrogram of O 1s, which confirms that the prepared oxygen vacancies are also conducive to improving the photocatalytic performance.41
9BiO2−x composite. As shown in Fig. 4(a), it can be seen that BiO2−x has a large and wide peak with g = 2.05.10,37–39 This is attributed to bismuth defects caused by oxygen vacancies in the photocatalytic material. The EPR signal becomes stronger after compositing, indicating that the oxygen vacancy concentration increases after compositing, which is also conducive to the improvement of photocatalytic degradation performance. The embedded figure is a comparison between the enlarged yellow region of the composite material and the EPR of the COF. It can be clearly seen from the figure that the COF can detect vibration signals at g = 2.003, indicating that the COF also has oxygen vacancies,40 and the EPR signal of the composite has a wide peak of bismuth defects caused by oxygen vacancies at g = 2.05. There is also an oxygen vacancy peak of g = 2.004. It is further proved that the composite material has oxygen vacancies. This conclusion is consistent with the previous XPS spectrogram of O 1s, which confirms that the prepared oxygen vacancies are also conducive to improving the photocatalytic performance.41
The optical properties of BiO2−x, the COF and the 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x composite can be obtained from UV-visible diffuse reflectance spectra (DRS), the light absorption intensity and the range of the catalyst can be evaluated, and the band gap of the corresponding materials can be calculated according to the Tauc plot formula. The redshift of the strongest absorption peak of the composite material was obtained from Fig. 4(b), and the light absorption capacity of the composite material was enhanced compared with that of pure BiO2−x, indicating that its absorption of visible light was also improved. Fig. 4(c) and (d) show the band gap widths (Eg) of the COF and BiO2−x calculated according to the Tauc plot formula, which are 2.26 eV and 1.62 eV, respectively.
9BiO2−x composite can be obtained from UV-visible diffuse reflectance spectra (DRS), the light absorption intensity and the range of the catalyst can be evaluated, and the band gap of the corresponding materials can be calculated according to the Tauc plot formula. The redshift of the strongest absorption peak of the composite material was obtained from Fig. 4(b), and the light absorption capacity of the composite material was enhanced compared with that of pure BiO2−x, indicating that its absorption of visible light was also improved. Fig. 4(c) and (d) show the band gap widths (Eg) of the COF and BiO2−x calculated according to the Tauc plot formula, which are 2.26 eV and 1.62 eV, respectively.
After the successful synthesis of the material, which was confirmed by the characterization method, the performance of the catalyst was tested. Under visible light irradiation, diclofenac was photocatalyzed to evaluate the photocatalytic performance of composites with different weight ratios, and DCF was quantitatively analysed using high-performance liquid chromatography. As shown in Fig. 5(a), the composite ratio with the best photocatalytic degradation performance is 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9, and with an increase in the amount of COF, the adsorption in the dark reaction stage is enhanced, which is also attributed to the advantage of the large specific surface area of the COF. The degradation rate of the composite ratio of 1
9, and with an increase in the amount of COF, the adsorption in the dark reaction stage is enhanced, which is also attributed to the advantage of the large specific surface area of the COF. The degradation rate of the composite ratio of 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9 reaches 96% at 60 min and 97% at 90 min, and the optimal composite ratio is 1
9 reaches 96% at 60 min and 97% at 90 min, and the optimal composite ratio is 1![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9. Compared with BiO2−x, the photocatalytic performance of the 1COF
9. Compared with BiO2−x, the photocatalytic performance of the 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x composite is better. Blank control experiments were also conducted to confirm the importance of illumination (Fig. S3†).
9BiO2−x composite is better. Blank control experiments were also conducted to confirm the importance of illumination (Fig. S3†).
In addition to assessing the photocatalytic efficacy, the kinetics of DCF degradation under photocatalysis was investigated. It was postulated that the degradation of DCF by different materials follows first-order reaction kinetics, and kinetic modeling was conducted based on the corresponding rate equations.
The degradation of diclofenac was similarly assumed to adhere to first-order kinetics and was fitted accordingly using the kinetic equation. As shown in Fig. 5(b), the degradation kinetics is first-order, the reaction rate constant is obtained, and the reaction rate constant of the 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x composite is the highest.
9BiO2−x composite is the highest.
In addition to evaluating the photocatalytic performance of the catalyst, its stability is also an important property for long-term use in practical applications. In order to assess the stability of the composite photocatalyst, the recycling experiment was performed four times over the composite. As shown in Fig. 6(a), the material can be recycled four times, and the photocatalytic degradation performance of the 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x composite decreases after four cycles, which may due to the loss of some solids in each cycle experiment. The amount of the photocatalyst is reduced. However, 97% of the degradation effect is still achieved after four cycles, indicating that the catalyst shows good physical and chemical stability and good recyclability. In order to better verify this, XRD and IR were conducted after four cycles, as shown in Fig. 6(b) and (c). It can be seen that the IR data and XRD patterns of 1COF
9BiO2−x composite decreases after four cycles, which may due to the loss of some solids in each cycle experiment. The amount of the photocatalyst is reduced. However, 97% of the degradation effect is still achieved after four cycles, indicating that the catalyst shows good physical and chemical stability and good recyclability. In order to better verify this, XRD and IR were conducted after four cycles, as shown in Fig. 6(b) and (c). It can be seen that the IR data and XRD patterns of 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x before and after four cycles are basically consistent, indicating that the catalyst has good stability, which is of great value for the practical application of the material.
9BiO2−x before and after four cycles are basically consistent, indicating that the catalyst has good stability, which is of great value for the practical application of the material.
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| Fig. 6  (a) 1COF ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) : ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x catalysed by visible light for 4 cycles and FT-IR spectra (b) and XRD patterns (c) of 1COF ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) : ![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x obtained before and after the reaction. | ||
To elucidate the mechanism behind the improvement of photocatalytic activity, two main factors affecting the photocatalytic performance of light absorption and charge separation were studied. The photochemical properties of the catalyst were assessed using the transient photocurrent response and electrochemical impedance spectroscopy (EIS). The transient photocurrent value provided a direct indication of the separation efficiency and migration rate of the photoinduced charge carriers. Fig. 7(a) shows that the transient photocurrent response of 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x increases significantly, showing the best photoresponse performance, which proves that under visible light irradiation, 1COF
9BiO2−x increases significantly, showing the best photoresponse performance, which proves that under visible light irradiation, 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x has higher carrier separation efficiency than BiO2−x.
9BiO2−x has higher carrier separation efficiency than BiO2−x.
The results of electrochemical impedance spectroscopy and photocurrent density test are consistent, indicating that the effective electron transfer in 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x is the main reason for its excellent photocatalytic activity. EIS is commonly used to study the separation efficiency of electrons and holes in photocatalytic reactions. As shown in Fig. 7(b), the EIS Nyquist plot of the 1COF
9BiO2−x is the main reason for its excellent photocatalytic activity. EIS is commonly used to study the separation efficiency of electrons and holes in photocatalytic reactions. As shown in Fig. 7(b), the EIS Nyquist plot of the 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x composite is significantly smaller than that of other composites, indicating that after the appropriate combination of BiO2−x and the COF, the charge transfer resistance is reduced and the photogenerated electrons and hole recombination rate are reduced, which proves that the improvement of its photocatalytic ability under visible light promotes the photocatalytic degradation reaction. In addition, fluorescence photoluminescence spectra can be used to evaluate the electron and hole recombination efficiency of the material, and the stronger the fluorescence intensity, the more easily the photogenerated electrons and holes recombine. As shown in Fig. 7(c), comparatively, it can be clearly found that the PL emission intensity of the composite (1COF
9BiO2−x composite is significantly smaller than that of other composites, indicating that after the appropriate combination of BiO2−x and the COF, the charge transfer resistance is reduced and the photogenerated electrons and hole recombination rate are reduced, which proves that the improvement of its photocatalytic ability under visible light promotes the photocatalytic degradation reaction. In addition, fluorescence photoluminescence spectra can be used to evaluate the electron and hole recombination efficiency of the material, and the stronger the fluorescence intensity, the more easily the photogenerated electrons and holes recombine. As shown in Fig. 7(c), comparatively, it can be clearly found that the PL emission intensity of the composite (1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x) exhibited a significant decrease in recombination, indicating that the coupling of BiO2−x and the COF effectively suppressed the recombination of photogenerated electron–hole pairs.42
9BiO2−x) exhibited a significant decrease in recombination, indicating that the coupling of BiO2−x and the COF effectively suppressed the recombination of photogenerated electron–hole pairs.42
Before the mechanism of photocatalytic oxidation of DCF was proposed, free radical trapping experiments and EPR were performed to determine the types of active species and their respective contributions. In these trapping experiments, EDTA disodium salt (EDTA-2Na) was used to trap photogenerated h+, isopropyl alcohol (IPA) was used to trap hydroxide radicals (˙OH), and vitamin E and AgNO3 were selected to trap the superoxide anion radical (˙O2−) and e−, respectively. As shown in Fig. 7(d), the degradation rate of diclofenac decreased when EDTA-2Na and vitamin E were added to the photocatalytic reaction, and the main active species of diclofenac were h+ and ˙O2−. Moreover, after adding AgNO3, the degradation rate of the photocatalyst was improved, indicating that the content of h+ increases after the trapping agent captures e−, so the photocatalytic rate increases, which also reflects that h+ is the main active species.
Under simulated experimental conditions, the existence of ˙O2− radicals in the reaction system was confirmed by electron spin resonance (EPR). As shown in Fig. 7(e), almost no signal was observed when the system was in the dark, indicating that 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x could not produce ˙O2− under dark conditions. The EPR signal of DMPO-˙O2− can be clearly observed after 5 min of illumination, and the signal intensity of DMPO-˙O2− increases with the increase of illumination time. The results indicated that 1COF
9BiO2−x could not produce ˙O2− under dark conditions. The EPR signal of DMPO-˙O2− can be clearly observed after 5 min of illumination, and the signal intensity of DMPO-˙O2− increases with the increase of illumination time. The results indicated that 1COF![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) :
:![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 9BiO2−x could produce ˙O2− under illumination. As shown in Fig. 7(f), DMPO-˙OH was not detected under either dark or light conditions, indicating that the catalyst could not produce ˙OH. This is consistent with the results obtained from the trapping experiments.
9BiO2−x could produce ˙O2− under illumination. As shown in Fig. 7(f), DMPO-˙OH was not detected under either dark or light conditions, indicating that the catalyst could not produce ˙OH. This is consistent with the results obtained from the trapping experiments.
After identifying the active species, Mott–Schottky (M–S) analysis and valence band XPS spectra were employed to calculate the relative positions of the conduction band (CB) and the valence band (VB) of the COF and BiO2−x. As shown in Fig. S4(a) and (b),† the slope of M–S is positive, indicating that BiO2−x and the COF are n-type semiconductors. This shows that the Fermi level (EF) is equivalent to the flat band potential (Efb).43 The Mott–Schottky plots, which mean the Fermi energy level (EF) of BiO2−x and the COF, can be obtained from the intercept on the horizontal coordinate as −0.53 eV and −0.51 eV (vs. Ag/AgCl) (−0.31 eV and −0.29 eV (vs. NHE)), respectively. The distance between the maximum value of the VB and the Fermi level can be determined by the valence band XPS spectra, as shown in Fig. S5(a) and (b).†![[thin space (1/6-em)]](https://www.rsc.org/images/entities/char_2009.gif) 33 The distance between BiO2−x and the COF is about 0.80 eV and 1.70 eV, respectively. The VB potentials of BiO2−x and the COF are 0.49 eV and 1.41 eV (vs. NHE), respectively, and the CB potentials are −1.13 eV and −0.85 eV (vs. NHE), respectively.34,44 The band potentials of BiO2−x and the COF exhibit a staggered band alignment, resulting in an energy bias naturally generated at the contact interfaces between these materials in the composite. This energy bias facilitates the separation and transfer of photogenerated carriers in the system.
33 The distance between BiO2−x and the COF is about 0.80 eV and 1.70 eV, respectively. The VB potentials of BiO2−x and the COF are 0.49 eV and 1.41 eV (vs. NHE), respectively, and the CB potentials are −1.13 eV and −0.85 eV (vs. NHE), respectively.34,44 The band potentials of BiO2−x and the COF exhibit a staggered band alignment, resulting in an energy bias naturally generated at the contact interfaces between these materials in the composite. This energy bias facilitates the separation and transfer of photogenerated carriers in the system.
According to the above experimental results and discussion, the photocatalytic degradation mechanism of BiO2−x/COF on DCF in water was proposed. As shown in Fig. 8, under visible light irradiation, both the COF and BiO2−x can be excited, generating e− and h+. Due to the band energy difference between the COF and BiO2−x, photogenerated electrons in the conduction band (CB) of BiO2−x tend to migrate to the CB of the COF, while h+ in the valence band (VB) of the COF move to the VB of BiO2−x. This directional carrier migration effectively inhibits the recombination of electron–hole pairs and enhances the photocatalytic activity of the whole system. In addition, considering that CB potentials of BiO2−x and the COF (−1.13 eV and −0.85 eV) are more negative than those of Eθ (O2/˙O2−) (−0.33 eV vs. NHE), the electrons in the CB of the COF can be reduced to ˙O2− through a one-electron reducing reaction. The DCF adsorbed on the surface of the BiO2−x/COF catalyst is oxidized and degraded under the action of ˙O2−, while the strong oxidizing h + located on the VB of BiO2−x can directly oxidize and degrade DCF. The DCF in the final aqueous solution is degraded by the joint action of h+ and ˙O2−, thus achieving the removal of pollutants. In the BiO2−x/COF photocatalyst, the introduction of oxygen vacancies on BiO2−x leads to the reduction of the band gap width of the catalyst, and therefore has a wider range of wavelength response, while the COF acts as a high-quality carrier based on its adsorption performance, carrier transport performance and the presence of oxygen vacancies. The photocatalytic degradation performance of the two materials was improved by forming a traditional type-II heterojunction.
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| Fig. 8 Mechanism diagram of the photocatalytic degradation of DCF by the BiO2−x/COF heterojunction under visible light irradiation. | ||
In the evaluation stage of photocatalytic performance, by-products were observed in the degradation process. Based on the kinetic results and the peak conditions (Fig. S6†) of LC-MS, we proposed the mechanism of photocatalytic degradation of DCF, as shown in Scheme 2.45–49 LC-MS analysis was conducted to determine the formation of photocatalytic intermediates during the irradiation process. In the photocatalytic reaction, BiO2−x/COF is stimulated by light to produce more reactive oxygen species, and the effect of oxidative decarboxylation is enhanced. Diclofenac is preferentially oxidized and decarboxylated to 2,6-dichloro-N-o-tolyaniline (m/z = 252) under hydroxylation addition, and then produces m/z 234 and 199 products under dechlorination and oxidation. Another degradation pathway was oxidative decarboxylation to 2,6-dichloro-N-o-tolyaniline (m/z = 252) and dechlorination to an m/z of 218.07 and an m/z of 184.11. These intermediates are eventually degraded into small molecules (m/z = 161.99, m/z = 94, m/z = 61) as well as CO2 and H2O.
| Footnote | 
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4nr00608a | 
| This journal is © The Royal Society of Chemistry 2024 |