Aleena Majeeda,
Samna Hassana,
Musarrat Zahraa,
Iqra Rafiqueb,
Sajid Iqbal
c,
Munib Ahmad Shafiqd,
Rashid Nazir Qureshid,
Ramzan Akhtar
e,
Muhammad Rehanf,
Mohsin Ali Raza Anjume,
Sheeraz Mehboobe,
Jaweria Ambreen
*ag,
Jae Ho Yun*h and
Muhammad Saifullah
*e
aDepartment of Chemistry, COMSATS University Islamabad, Park Road, 45550, Islamabad, Pakistan. E-mail: Jaweria.ambreen@comsats.edu.pk
bIsotope Production Division (IPD), Pakistan Institute of Nuclear Science and Technology (PINSTECH), P.O. Box 45650, Nilore, Islamabad, Pakistan
cDepartment of Nuclear and Quantum Engineering, Korea Advanced Institute of Science and Technology, Daejeon, South Korea
dCentral Analytical Facility Division (CAFD), Pakistan Institute of Nuclear Science and Technology (PINSTECH), Islamabad, Pakistan
eChemistry Division, Pakistan Institute of Nuclear Science and Technology (PINSTECH), Islamabad, Pakistan. E-mail: Saifi.551@gmail.com
fPhotovoltaic Research Department, Korea Institute of Energy Research (KIER), Daejeon, South Korea
gDepartment of Biomedical Engineering & Health Sciences, Faculty of Electrical Engineering, Universiti Teknologi Malaysia, 81310 UTM, Johor Bahru, Johor, Malaysia
hDepartment of Energy Engineering, Korea Institute of Energy Technology, South Korea. E-mail: jhyun@kentech.ac.kr
First published on 19th May 2025
The two-dimensional layered structure of g-C3N4 (GCN) has drawn a lot of attention in the field of photocatalysis due to its good thermochemical stability, large surface area, and environmental friendliness. A wide bandgap of GCN restricts its absorption to UV light and a limited portion of visible light; therefore, its bandgap engineering by coupling it with a suitable semiconductor can offer the utilization of a wider spectrum of incident light and a lower electron–hole recombination rate. In this study, GCN is coupled with mixed-phase Bi2O2CO3–Bi4O7 (BO) in different weight percentages (wt%) to find the optimal loading of BO for maximum photocatalytic degradation. The XRD analysis confirms the preparation of GCN, BO, and g-C3N4/Bi2O2CO3–Bi4O7 composites. The g-C3N4/Bi2O2CO3–Bi4O7 composite with 24 wt% of BO (CN/BO-24) demonstrates 92.3% rhodamine B (RhB) dye degradation in 25 min under visible light irradiation, which is considerably higher compared with the corresponding % degradation realized with pristine GCN (73.4%) and BO (9.4%). The improved performance of the composite with optimal loading of BO is attributed to the reduced recombination rate of photo-generated electrons and holes, as confirmed by photoluminescence analysis, and utilization of a wider spectrum of incident light. Photo-degradation experiments performed with different scavengers reveal that peroxide radicals and holes play a decisive role in the degradation of RhB using the best composite sample (CN/BO-24). The potential of the CN/BO-24 ternary composite for the photoreduction of Cr(VI) is also explored. The fabricated composite holds promising potential in water treatment and environmental remediation.
Many semiconductors, such as Fe2O3,9 SnO2,10,11 BiVO4,12 ZnS,13 Cu2O, and g-C3N414 have been extensively explored in photocatalysis. Besides the semiconductor photocatalysts mentioned above, TiO2 has been widely explored for its potential to degrade organic contaminants in aqueous solutions.15 Although TiO2 is a good photocatalytic material, its wide bandgap of 3.2 eV limits its ability to harness solar energy, as it primarily absorbs UV light below 400 nm. Using TiO2, only a small portion of incident solar light, falling mainly in the UV region, can be harnessed for targeted chemical reactions. Therefore, visible light-driven photocatalysts with narrow bandgap, or wide bandgap semiconductors coupled with narrow bandgap semiconductors, are preferred as they can utilize a wider spectrum of sunlight.15
Graphite carbon nitride, g-C3N4 (GCN), is currently being explored for different photocatalytic reactions such as H2 production, reduction of hexavalent chromium, CO2 photoreduction, and pollutant degradation.16,17 GCN is composed of stacked layers of the two-dimensional conjugated framework of s-triazine and has a bandgap of ∼2.7 eV.18 Researchers are drawn towards its exceptional characteristics, such as high thermal, chemical, and mechanical durability, favorable optoelectronic properties, and ecologically benign nature.19–21 However, pristine GCN has some drawbacks like partial absorption of visible light due to its wide bandgap and fast charge carriers' recombination, which limits its photocatalytic activity.18
To improve the photocatalytic performance of the pristine GCN, many efforts have been undertaken, including doping with heteroatoms and metals, construction of the mesoporous structure, copolymerization with organic molecules, and coupling with other semiconductors.22–25 The construction of its composite with other semiconductors holds great potential to improve its photocatalytic efficiency.26 A heterojunction is preferably created with a comparatively narrower bandgap material to overcome these drawbacks and enhance GCN's photocatalytic activity. The approach to form a composite with good interfacial contact between two semiconductors with well-matched electronic band structures not only widens the harnessable solar spectrum but also allows efficient charge transfer, which suppresses the recombination of photogenerated electrons and holes.27 The development of direct Z-scheme photocatalysts has received a lot of interest lately because of their ability to effectively separate photogenerated electron–hole pairs spatially and maximize the photocatalytic system's ability for reduction and oxidation reactions.28 Yu et al. (2013) introduced the idea of a direct Z-scheme photocatalyst to explain strong photocatalytic formaldehyde (HCHO) degradation using TiO2/GCN composite.29
A wide variety of binary heterojunction composites have been made between Ag3PO4,30 Bi2MoO6,31 BiOBr,32 NiTiO3,33 ZnO,34 MnO2,35 etc. and GCN. Pham and Shin (2018) reported NiTiO3/GCN composite as an excellent photocatalyst for photocatalytic CO2 reduction.33 Pradhan et al. (2021) communicated MnO2 modified exfoliated porous GCN nanosheet for enhanced photocatalytic oxidation efficiency of aromatic alcohols.18 Rashidizadeh et al. (2020) described a GCN/CuWO4 nanocomposite for the degradation of methylene blue.26 Vidyasagar et al. (2018) demonstrated (Ag/AgO) loaded GCN for degradation of acidic dyes and bacterial inactivation.36 The photocatalytic performance has been further improved by employing ternary composite materials.37 Liu et al. (2018) prepared a ternary composite GCN/Ag3PO4/Ag2MoO4 for producing oxygen from water splitting.38 Similarly, Tang et al. (2020) prepared a ternary composite AgI/Ag3PO4/g-C3N4 for the degradation of rhodamine B (RhB) under visible light irradiation.39
Bismuth subcarbonate (Bi2O2CO3) has garnered immense interest due to its chemical stability, non-toxicity, affordability, and environmental friendliness.40 Bi2O2CO3, existing in the sillén phase, has intergrown (Bi2O2)2+ and (CO3)2− layers with the orthogonal plane of (CO3)2− groups.41 The conduction band of GCN is more negative compared with Bi2O2CO3, while the valence band of Bi2O2CO3 is more positive relative to GCN.42,43 Making a composite of Bi2O2CO3 with GCN, therefore, is anticipated to improve photocatalytic performance by reducing charge carriers' recombination. However, the visible light absorption of GCN-Bi2O2CO3 composite is expected to remain limited as both Bi2O2CO3 and GCN have a wide bandgap of 2.4144 and 2.70 eV,45 respectively. To improve visible light absorption and thereby enhance photocatalytic activity, making a mixed phase of Bi2O2CO3 with Bi4O7, which has a narrow bandgap of 1.89 eV
46 and coupling it with GCN can be effective. This novel approach of making a composite of mixed-phase Bi2O2CO3–Bi4O7 with GCN will bring the advantage of enhanced photocatalytic activity due to extended absorption of the incident spectrum and increased availability of photo-generated carriers.
In this paper, we report the preparation of ternary composite, g-C3N4/Bi2O2CO3–Bi4O7, photocatalysts with varying weight percentages of Bi2O2CO3–Bi4O7. The photocatalytic activities of g-C3N4/Bi2O2CO3–Bi4O7 composites are evaluated against RhB degradation and the photoreduction of Cr(VI) under visible light irradiation. The composite sample, having 24 wt% Bi2O2CO3–Bi4O7, i.e., optimal loading, demonstrated 92.3% of RhB degradation in just 25 min under visible light irradiation. The degradation performance of this composite is considerably better compared with both GCN (73.4%) and Bi2O2CO3–Bi4O7 (9.4%).
Fig. 2 shows the XRD diffractograms of as-synthesized GCN, BO, and CN/BO composites with 10, 17, 24, and 30 wt% of BO. XRD pattern of GCN, as can be seen in Fig. 2, clearly shows two distinctive diffraction peaks at 13.1 and 27.4° that can be indexed to the (002) and (100) crystal planes, respectively (PDF card no. 087-1526). The XRD analysis of BO indicates its successful synthesis, i.e. mixture of Bi2O2CO3 and Bi4O7. The composite or mixed phase of these materials as a photocatalyst has been reported to perform better compared with the phase-pure Bi2O2CO345 and Bi4O7.15 In Bi2O2CO3, peaks at 12.9, 23.9, 26.0, 30.2, 32.7, 39.5, 42.2, 46.9, 52.2, 53.4, and 56.8° correspond to (002), (011), (004), (013), (110), (006), (114), (020), (116), (121), and (123) planes, respectively, of PDF card no. 00-041-1488. In addition, other peaks at 27.6, 28.3, and 31.3° corresponding to (2−2−2), (22–2), and (400) planes, respectively, are also observed. These characteristic peaks belong to Bi4O7 with PDF card no. 00-47-1058. In BO, the majority of observed peaks belong to Bi2O2CO3, whereas only a few peaks are found for Bi4O7. Liu et al. (2021) reported that high-temperature processing of Bi2O2CO3 converts it into the corresponding oxide phases.15 In this study, the formation of Bi2O2CO3–Bi4O7 mixed phase can be attributed to high temperature and pressure conditions during hydrothermal reaction and annealing at 250 °C during the composite preparation step. For fair comparison of BO with composite samples, BO after its synthesis by the hydrothermal method is also subjected to annealing at 250 °C. Because of the overlapping of the diffraction peaks for Bi4O7 (27.6°) and g-C3N4 (27.4°), it is difficult to distinguish their individual peak. Ge et al. (2011) have also observed a similar overlapping of diffraction peaks in g-C3N4/Bi2WO6.49 Most of the peaks correspond to Bi2O2CO3 in all the composites, indicating that both Bi4O7 and Bi2O2CO3 phases are present. Therefore, it can be concluded that the composites contain GCN, Bi4O7, and Bi2O2CO3.
FTIR analysis is performed to examine different vibration modes in pristine GCN, BO, and the prepared CN/BO composites. The resulting FTIR spectra are displayed in Fig. 3. Pure GCN exhibits its distinctive vibration peaks at wave numbers of 808, 1230, 1313, 1537, 1632, and 3185 cm−1, which is in accordance with results reported by Tian et al. (2014).45 The wide band at 3185 cm−1 appears to be related to the –OH groups, most likely due to adsorbed water molecules and the stretcting vibrations of –NH groups.50,51 The triazine units yielded a peak at 808 cm−1, whereas the stretching vibration of the C–N heterocyclic is reflected between 1233 to 1537 cm−1. The C–N and CN stretching modes are represented by the peaks at 1313 and 1632 cm−1, respectively.51 Regarding the BO, the stretching vibrations of the Bi–O–Bi in the compound are responsible for a peak at about 849 cm−1, whereas the stretching vibrations of C–O and C
O are manifested in a form of broad peaks at around 1400 cm−1.15
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Fig. 3 FTIR patterns of pristine GCN and BO, as well as composites CN/BO-10, CN/BO-17, CN/BO-24, and CN/BO-30. |
In the case of CN/BO composite samples (CN/BO-10, CN/BO-17, CN/BO-24, and CN/BO-30), the FTIR spectra display a combination of vibrational features from both GCN and BO components, confirming successful composite formation. All CN/BO composites exhibit peaks in the region of 1233–1537 cm−1, indicating the retention of C–N stretching modes, and the peak around 1632 cm−1 denoting the CN stretching. A difference that is visible in composite samples compared with the pristine GCN and BO is the emergence of a peak at 2362 cm−1 which arises from the stretching vibration of surface-adsorbed CO2.52 The CO2 in composite samples comes from the decomposition of CO3 in Bi2O2CO3, which gets adsorbed in high surface area GCN. A high surface area of GCN is confirmed from the BET analysis which will be discussed in Section 3.2. A similar vibration peak originating from CO2 does not emerge in BO, most probably because of its small surface area. To confirm the successful composite formation, selected regions of FTIR patterns of only GCN and CN/BO-24 are shown in Fig. S1.† On having a close look at the 1233–1537 cm−1 region in Fig. S1(a),† it is observed that peaks related to s-trizine system are red-shifted. For instance, 1205, 1230, 1397, 1455, and 1537 cm−1 are shifted to lower wavenumbers. Such a red shift in FTIR peaks of GCN in the composite samples originates from the electronic interaction between the two constituents of the composite. The nitrogen sites in GCN can interact with Bi cations in BO, which act as a Lewis acid, while nitrogen functions as a Lewis base. The other possible interaction that in parallel can lead to such a red shift is the hydrogen bonding between amines in GCN and CO3−2 functionalities in the Bi2O2CO3. These interactions result in the weakening of C–N bonds in GCN. Fig. S1(b)† shows that another peak at 808 cm−1 in the composite (i.e. CN/BO-24) relating to GCN triazine units bending vibration is also red-shifted.53 These spectral changes collectively confirm the successful formation of a well-integrated CN/BO composite with strong interfacial interactions and altered vibrational properties.
To assess the separation efficiency and the degree of recombination of the photogenerated electrons and holes in GCN and CN/BO composite, photoluminescence (PL) analysis is performed. The PL emission gets intense as the photogenerated carriers' recombination efficiency in a semiconductor increases.45 Therefore, the photocatalytic material's performance will be compromised due to the lower availability of carriers. The PL spectra of the pristine GCN as well as composite samples (i.e. CN/BO-10, CN/BO-17, CN/BO-24, and CN/BO-30) are shown in Fig. 4. It can be observed in Fig. 4 that GCN has an emission peak at a wavelength (λ) of 456 nm. This emission wavelength corresponds to a bandgap (Eg) of 2.72 eV, which is in accordance with the literature.45 On adding BO to GCN for up to 24 wt%, the PL emission intensity gradually decreases, which can be attributed to the reduced recombination of photogenerated carriers in composite samples. Tian et al. (2015) also reported a decrease in the intensity of PL spectra by BiVO4/g-C3N4 composite, which was attributed to reduced charge carrier recombination as compared to GCN.54 On further increasing the BO content in GCN up to 30 wt%, PL emission again gets intense, and the peak intensity becomes almost equivalent to that of GCN. This reversal of trend in the PL emission intensity suggests that, in terms of carriers' lifetime, the best composite sample is CN/BO-24, and the approach to couple GCN with BO seems to bring positive implications toward photocatalytic performance. The results on the photocatalytic performance as a function of BO loading in CN/BO composite will be presented in the proceeding section.
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Fig. 4 Photoluminescence spectra of pristine GCN, BO, CN/BO-10, CN/BO-17, CN/BO-24, and CN/BO-30 composites taken with a He–Ne laser with excitation wavelength 325 nm. |
The elemental composition analysis of GCN, BO, CN/BO-10, CN/BO-17, CN/BO-24, and CN/BO-30 is also performed to check if the GCN retains its structure in composite samples. GCN is primarily composed of carbon and nitrogen, forming a polymeric structure of triazine units. The N/C molar ratio in the prepared GCN is found to be 1.54, which is higher than what one could expect in C3N4, i.e., 1.33. Nithya and Ayyappan (2020) also reported an N/C molar ratio of 1.47 for GCN.55 In pristine BO, 0.94% of C is detected, suggesting the presence of Bi2O2CO3 in addition to Bi4O7. This once again validates the results of the XRD analysis. Additionally, it also has 13.69% of O content. In the composite samples, the N/C ranges from 1.52 to 1.54 and shows only a small variation between samples. This implies that GCN stoichiometry has not changed considerably during the composite preparation step. Further, the relatively higher percentage content of C and N in the composite suggests that GCN acted as a matrix in the composite samples.
The thermal stability of GCN is assessed by thermogravimetric analysis (TGA), as shown in Fig. S2.† The TGA analysis indicated that GCN remains stable up to 500 °C. Differential thermogravimetric analysis (not shown) revealed that GCN showed a peak at 638 °C, which can be attributed to its degradation. Wang et al. (2012) also reported a peak at 630 °C in GCN.56 This indicates that GCN retains its structure during the preparation of composite samples through the annealing process carried out at 250 °C, which is also corroborated by the CHNS-O analysis discussed above.
Both improved separation of photogenerated carriers and increased visible light absorption seem responsible for boosting the photocatalytic activity of CN/BO-24. Therefore, the ideal concentration of BO in GCN for a composite photocatalyst is 24%, where the optimum combination for both light absorption and charge transfer is achieved. Increasing the BO loading in GCN to 30% might increase the light absorption, however, the charge transfer and the reaction at the surface of the catalyst will be limited due to the low concentration of GCN and possible aggregation of BO and its low surface area. This may badly impact the photocatalytic performance. In Fig. 5(b), it is evident that the CN/BO-24 composite demonstrates superior degradation performance, achieving almost complete degradation within just 25 min, with a degradation performance of approximately 92.3%. This suggests that the combination of BO and GCN in the CN/BO-24 composite effectively suppresses charge carrier recombination, enhancing its photocatalytic efficiency.
To assess the available surface area (SA) of the prepared photocatalysts, BET analysis of pristine samples, GCN, and BO is performed. This measurement can reveal any existing correlation between the enhanced photocatalytic performance and the SA of the composite. The SA is found to be 38.7835 m2 g−1 for GCN and 1.4526 m2 g−1 for BO (data not shown). Following the wt% ratio of the GCN and BO in the best-prepared composite CN/BO-24, the theoretical SA is determined to be 30.1687 m2 g−1, which is lower compared to the SA of GCN. Although SA can influence the number of active sites available for dye adsorption and degradation, photocatalytic performance is often more strongly governed by charge carrier dynamics, especially in reactions involving visible light-driven processes. The superior activity of the composite, i.e. CN/BO-24, can be attributed to enhanced charge separation and reduced recombination rate, which are likely a result of favorable synergistic electronic interactions at the GCN–BO interface. The efficient charge transfer prolongs the lifetime of charge carriers, making them more available for dye degradation. The PL study, as shown in Fig. 4, also indicates the low charge carriers' recombination of the CN/BO-24 composite.
To study the kinetics of the photo-degradation process, data is fitted with a pseudo-first-order kinetics equation, ln(C/Co) = −kt, where C0 is the initial concentration, C is the concentration at different time intervals, k is the kinetic constant, and t is the time. The fitted data, shown in Fig. 5(d), indicate that the photo-degradation process of the prepared catalysts follows a pseudo-first-order kinetics. The values of k for the prepared catalysts are presented in Fig. 5(e). The degradation rate constant of GCN and BO for RhB in the degradation process is 0.054 and 0.001 min−1, respectively, again indicating that the photocatalytic efficiency of GCN is better in comparison to BO. The values of k for CN/BO-10, CN/BO-17, CN/BO-24, and CN/BO-30 are 0.060, 0.065, 0.107, and 0.041 min−1, respectively. Fig. 4(d) shows that the kinetic constant k of CN/BO-24 degradation is about 2 and 72 times higher than that of pure GCN and BO, respectively.
An additional crucial factor for the practical use of the produced photocatalyst in environmental applications is its regenerative stability under light irradiation. Fig. 6(a) illustrates the RhB photo-degradation profiles versus time with CN/BO-24 composite in the three successive runs. The percentage degradation of RhB in 45 min in the first, second, and third runs is 98.3, 85.8, and 73.0%, respectively, which indicates a slight decrease in repetitive use. To verify any potential phase changes in the catalyst following photocatalytic degradation, XRD analysis is conducted, as shown in Fig. S3.† The results indicate that the catalyst retains the same phase before and after the photocatalytic activity, demonstrating the stability of the prepared photocatalyst.
Ultimately, by combining the previously determined bandgap values, as well as the conduction band (CB) and valence band (VB) position of pure components, an energy band diagram of the potential ternary composite photocatalytic process can be anticipated. Fig. 7 shows the potential photodegradation schematic mechanism in a ternary heterojunction structure. Under visible light irradiation, GCN, Bi4O7, and Bi2O2CO3 are all excited, leading to the generation of electron–hole pairs. However, the extent of photo-generation of carriers is controlled by the bandgap value, which is the lowest in Bi4O7. The electrons in the CB of Bi2O2CO3 (0.65 eV)44 recombine with holes in the VB of Bi4O7 (2.52 eV).46 Simultaneously, electrons in CB of Bi4O7 (0.63 eV) recombine with holes in the VB of GCN (1.57 eV).45 As a result, electrons accumulate in the CB of GCN (−1.13 eV), which has a more negative edge, while holes build up in the VB of Bi2O2CO3 (3.06 eV), which has a more positive VB edge. Since the CB edge of GCN is more negative, the photogenerated electrons that accumulate in the CB of GCN have strong reducing power and react with O2 to form O2.– radicals. These O2.– radicals contribute to the decomposition of RhB. Meanwhile, the holes that remain in VB of Bi2O2CO3 exhibit strong oxidizing ability and directly react to the RhB molecules, breaking them down into products.
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Fig. 7 Proposed photocatalytic degradation mechanism of organic contaminants (RhB) in the presence of CN/BO composite. The CB and VB potentials of Bi2O2CO3, GCN, and Bi4O7 are obtained from previous studies.44–46 |
Table 1 compares the effectiveness of GCN combined with other photocatalysts in the degradation of RhB dye. The photocatalysts are mentioned along with their RhB degradation percentage, the time required, and the active quenching agents. It is evident from Table 1 that the ternary g-C3N4/Bi2O2CO3–Bi4O7 composite exhibits better degradation of RhB within a short time, showing a notable improvement in photocatalytic efficiency compared with other reported binary composites.
Year | Composite photocatalyst | % Degradation of RhB | Time | Quenching agents | References |
---|---|---|---|---|---|
2014 | BiOCl/GCN | 99 | 60 min | h+, O2˙− | 57 |
2015 | BiVO4/GCN | 85 | 5 h | .OH, O2˙− | 54 |
2015 | SnO2/GCN | 98.7 | 100 min | h+, O2˙− | 58 |
2017 | WO3/GCN | ∼100 | 2 h | .OH, O2˙− | 59 |
2017 | GCN/TiO2 | 95.2 | 80 min | h+, O2˙− | 60 |
2024 | GCN/Bi2O2CO3–Bi4O7 | 98.3 | 45 min | h+, O2˙− | This study |
The release of chromium (Cr) from industrial effluents into the environment is a cause of pollution.61 Cr in the environment exists in two main oxidation states, Cr(VI) and Cr(III). Cr(VI) is carcinogenic, mutagenic, and can cause a variety of health issues, therefore, its release in the environment has to be controlled.62 In contrast, the toxicity of Cr(III) is relatively low. To limit the adverse effect of Cr on the environment, Cr(VI) needs to be reduced to Cr(III).63 In this study, the prepared catalysts are also checked for their efficacy against the photoreduction of Cr(VI).
Fig. 8(b) shows the photoreduction performance versus time as well as photoreduction efficiency (η) of Cr(VI) using GCN, BO, and CN/BO-24 after 120 min of visible light irradiation. It is evident from Fig. 8(a) that the reduction efficiency in the case of BO is comparatively poor, whereas GCN and CN/BO-24 exhibited relatively better performance. Fig. 8(b) further shows that after 120 min, the η values for GCN, BO, and CN/BO-24 are 23.2, 8.8, and 25.8%, respectively. The η value is found to be the highest for CN/BO-24. The reduction mechanism is closely linked to electron–hole separation efficiency facilitated by the ternary composite of GCN, Bi4O7, and Bi2O2CO3. A similar trend is observed in both Cr(VI) photoreduction and RhB degradation studies. The photogenerated electrons in the CB of GCN are vital in Cr(VI) reduction, as they provide the necessary reducing power to convert toxic Cr(VI) to Cr(III).
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Fig. 8 (a) Photocatalytic reduction of Cr(VI) to Cr(III) versus time and (b) percentage photocatalytic Cr(VI) reduction efficiency of GCN, BO, and CN/BO-24 after 120 min of visible light irradiation. |
The performance of the oxygen evolution reaction (OER) is also evaluated by using GCN, BO, and CN/BO-24, as shown in Fig. S4.† From the results, it can be concluded that GCN displays better electrochemical performance for OER, while the CN/BO-24 composite exhibits the best photocatalytic performance.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d5ra00969c |
This journal is © The Royal Society of Chemistry 2025 |