Mi Wua,
Hongzhao Wanga,
Haifang Mao*a,
Chaoyang Wanga,
Zhenbiao Donga,
Ting Tang*b,
Wei Zhenga,
Lehong Jina and
Jibo Liu*a
aSchool of Chemical and Environmental Engineering, Shanghai Institute of Technology, 100 Haiquan Road, Shanghai, 201418, China. E-mail: mhf@sit.edu.cn; jiboliu@sit.edu.cn; Tel: +86-21-60877281
bHangzhou Normal University, College of Medicine, 2318 Yuhangtang Road, Hangzhou, Zhejiang, China. E-mail: tangtinghnu@163.com
First published on 14th February 2022
According to the requirements for sustainable development, reclaiming fine chemicals from wastewater under mild conditions is an extremely significant line of research. A low-cost and high-efficiency polydentate chelate- and polymeric Co(II)-based complex (Co-L)-loaded C3N4 photocatalyst (Co-L/C3N4) was constructed and used to convert aromatic mandelic acids in wastewater at room temperature. The BET specific surface area increased from 28 m2 g−1 to 68 m2 g−1, indicating its excellent absorptive character. The light absorption range of Co-L/C3N4 reached 650 nm, while the band energy reduced to 2.30 eV, which caused a significant enhancement in photocatalytic activity. The conversion of substituted mandelic acids was more than 90% due to the photoactivity of Co-L/C3N4. Time-resolved PL spectra indicated the remarkable separation of the photogenerated electron–hole pairs in Co-L/C3N4. Furthermore, the UV-vis and in situ FTIR spectra indicated the formation of aldehyde groups in the selective oxidation process, which provided support for the plausible catalytic mechanism.
However, due to the outstanding water solubility of MADs, their highly efficient conversion has always been the focus of attention, especially under low MAD concentration.12 The conversion rate and aromatic aldehyde selectivity of MADs can reach 85% and 70–80%, respectively, when various nanoparticles, such as Bi(0), Co(II), and Cu(II), are employed to catalytically convert MADs in DMSO.13–17 During this process, the introduction of organic solvents causes potential environmental problems. Silica-encapsulated Cu–Al hydrotalcite (SECuAlHT) was developed as an efficient catalyst to catalytically oxidize 4-hydroxy-3-methoxymandelic acid in a.q. solution under mild conditions, which gave a 72% yield of 4-hydroxy-3-methoxybenzaldehyde.18 Without a doubt, the chemical oxidation efficiency towards the substrate was limited under low substrate concentration.
Considering that environmental pollution and the sustainable supply of green energy are the two main global challenges being faced in the current era, photocatalytic selective oxidation technology has become a focus of international attention as it has potential for development.19–22 Photocatalysis has been widely used in water splitting, the degradation of organic pollutants, CO2 conversion, selective organic synthesis, and so on.23–26 In order to reclaim useful products from wastewater with low energy consumption and high efficiency, photocatalytic technology has attracted extensive attention due to its advantages of clean and environmentally friendly character derived from the use of solar energy.27 Thanks to the advantageous non-polluting nature and low-energy consumption, heterogeneous photocatalysis has been widely used for the generation of clean energy and catalytic oxidation. Several aromatic aldehydes have been obtained from the corresponding alcohols by employing photocatalytic technology in the water medium at room temperature and atmospheric pressure.28 It has been widely used for the detoxification of water and the air and has become a very promising fine chemical synthesis method in recent years.29 Without a doubt, noble metal catalysts, such as Au, Ru, and Pd, can mediate efficient oxidation reactions due to the low-temperature or preferential oxidation of CO, alcohol oxidation and soot oxidation.30 However, high cost is the dominating disadvantage of noble metal-based catalysts, limiting their large-scale use. Thus, low-cost catalyst construction has immense potential. In recent decades, metal-free semiconductor polymer carbon nitride (C3N4) has attracted attention due to its unique and interesting physical and chemical properties, such as high working efficiency under visible and ultraviolet light, strong stability, non-toxicity, non-polluting nature.31–34 For further improvement of the photocatalytic activity of C3N4, many strategies have been adopted, including doping with different metals, such as palladium, silver, and cobalt.35–38 Based on the principles of green sustainable chemistry and engineering, considerable efforts have been made to adjust the catalytic activity of C3N4 toward achieving excellent conversion and selectivity in aqueous solutions.39 Simultaneously, metal–organic complexes have attracted the attention of scientists due to their excellent catalytic activity and tunable structure. Considering that C3N4 exhibits excellent electron-transition ability due to the π-conjugated system, supporting π-conjugated compounds on C3N4 has been used to develop hybrid photocatalysts for selective photocatalytic oxidation in the fields of water splitting and organic synthesis.40,41 Especially, the usage of industrial solid waste for organic ligand synthesis can further realize the resource utilization of industrial by-products. For example, 5-aldehyde vanillin (5-AV) is the typical by-product formed during the production of vanillin. The oxhydryl and aldehyde groups make it an abundantly tuneable structure (Scheme 1).
Herein, a polydentate chelate and polymeric metal–organic complex based on 5-AV, a by-product of vanillin, was constructed and doped on the surface of C3N4 (Co-L/C3N4) to achieve the selective conversion of a variety of substituted mandelic acids to aromatic aldehydes efficiently under mild photocatalytic conditions. The conversion of the substrate reached 96.3% with an 84% selectivity. More importantly, the plausible mechanism for aromatic aldehyde production was investigated by employing in situ IR and UV-vis spectroscopy.
Then, 5-aldehyde vanillin (5.5 mmol, 1.0 g) and 1,3-diaminopropane (5.5 mmol, 0.41 g) were completely dissolved in ethanol (30 mL) under vigorous stirring at 75 °C and refluxed for 4 h. After it cooled down to room temperature, the solvent was evaporated to give ligand (L) as a white solid. The ligand (219 mg, 1 mmol) and CoCl2·6H2O (238 mg, 1 mmol) were added to EtOH (10 mL) and heated to 80 °C for 3 hours. After they cooled down to room temperature, the solvent was removed in a vacuum to get the Co(II) complex (Co-L). A certain amount of Co-L was mixed with C3N4 uniformly and calcined at 500 °C for 2 hours to obtain the Co/C3N4 catalyst (0.05 g Co-L mixed with 1 g C3N4 is denoted as Co-L/C3N4-5).
The crystalline structures of C3N4 and Co-L/C3N4 were examined by X-ray diffraction (XRD). As shown in Fig. 2a, the peaks at 13.5° and 27.2° were ascribed to the reflections of the (100) and (002) planes of C3N4, respectively.42 Interestingly, the peaks at 13.5° and 27.2° barely appeared in Co-L/C3N4, and these peaks became sharper and more obvious with the gradual increase in the Co-L ligand content, reflecting the enhanced crystallinity of the Co-L/C3N4 structure.36,43 The XRD results further confirmed the successful preparation and high stability of the Co-L/C3N4 heterostructure.44 In addition, the FT-IR spectra of the C3N4 and Co-L/C3N4 samples (Fig. 2b) exhibited some strong absorption peaks at 808 cm−1, which was the characteristic vibration of the out-of-plane bending of the triazine rings. The peaks at 1200–1650 cm−1 were attributed to the C–N and CN heterocycles, and those between 3000–3500 cm−1 could be assigned to the N–H/O–H groups. Interestingly, Co-L/C3N4 had a characteristic band similar to C3N4, indicating that the typical graphite structure of the carbonitride was not destroyed after Co-L doping. However, the peak at around 3100–3400 cm−1 was much narrower than that in the C3N4 spectrum, while the intensity was much greater, which is completely consistent with the description in the literature.45–47
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Fig. 2 (a) X-ray diffraction (XRD) patterns of C3N4 and Co/C3N4; (b) FT-IR spectra of C3N4 and Co/C3N4. |
To further investigate the surface microstructure of Co-L on the C3N4 nanoparticles, XPS (X-ray photoelectron spectroscopy) characterization was employed to investigate the constitution of the C3N4 and Co-L/C3N4-10 photocatalysts. As shown in Fig. 3a, both the C3N4 and Co-L/C3N4 samples consisted of C and N elements. Furthermore, a peak for Co appeared in the Co-L/C3N4 photocatalyst. In the high-resolution XPS analysis, the C 1s (Fig. 3b) deconvoluted peaks were centred at 284.5, 286.2 and 288.1 eV.48,49 The peak at 284.5 eV was ascribed to the physically adsorbed carbon species or the sp2 C–C bonds, and the peak at 286.2 eV was assigned to the C–NH2 species, while the strong peak at 288.1 eV could be attributed to N–CN. The three peaks at binding energies 398.6, 400.4 and 404.5 eV could be attributed to the triazine rings N–C
N, C2–N–H and C–N–H, respectively (as shown in Fig. 3c), which belong to the typical N 1s peaks in C3N4.50–53 In the high-resolution XPS analysis, the Co 2p peak at (Fig. 3d) the binding energy of 781.2 and 796.2 eV could be attributed to the Co(II) state in the form of Co–N. This indicated that the valence state of the Co ion in Co-L/C3N4 was Co(II) rather than Co(III). As shown in Fig. S5,† the Co 2p spectrum could be divided into Co2+ and Co3+ fitting curves, and four shakeup satellites. The fitting peaks at 782.5 and 797.4 eV could be grouped to Co3+, whereas the peaks at 779.5 and 794.5 eV were assigned to Co2+.38,54–56
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Fig. 3 (a) X-ray photoelectron spectroscopy (XPS) of C3N4 and Co-L/C3N4-15; (b–d) high-resolution XPS spectra of C 1s, N 1s and Co 2p. |
The N2 adsorption–desorption isotherms and pore size distribution curves of C3N4 and Co-L/C3N4-10 were recorded by the BET method, as shown in Fig. 4. All the prepared samples exhibited typical type IV isotherms and H3 hysteresis loops (Fig. 4a), implying the remarkable mesoporous properties of the materials.57 As a typical porous material, the specific surface area of C3N4 was 28 m2 g−1. As expected, the specific surface area of all the catalysts increased from 28 m2 g−1 to 86 m2 g−1 following the addition of 15% Co-L. The increase in specific surface area after Co doping was mainly due to the rich pore structure. As shown in Fig. 4b, the pore size and pore volume of the Co-L/C3N4 catalyst were larger than those of C3N4.58
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Fig. 4 (a) N2 adsorption–desorption isotherms of C3N4 and Co-L/C3N4; (b) the corresponding pore size distribution curves of C3N4 and Co-L/C3N4. |
The optical properties of the as-prepared photocatalysts were characterized by UV-vis diffuse reflectance spectroscopy (DRS). The DRS curves of the as-prepared C3N4 and Co-L/C3N4 samples are shown in Fig. 5a; C3N4 showed an absorption edge at ∼450 nm, suggesting its limited photo-response to visible light. More importantly, the absorption edge of Co-L/C3N4 was obviously red-shifted in comparison with C3N4.59 The optical absorption intensity of Co-L/C3N4 was significantly enhanced in the range of 550–650 nm. These results describe that Co doping facilitates secondary absorption in the visible light region, which would promote absorption in the wider range of visible light and the absorption efficiency of the system, resulting in higher photocatalytic activity.60,61 To further investigate the effect of Co doping on the optical bandgap energy of Co-L/C3N4, the Kubelka–Munk method was used to calculate the bandgap of the prepared samples.62 As shown in Fig. 5b, the presence of the Co-L ligand slightly reduced the energy band of C3N4. The results show that the Co-L ligand presented a good optical response in the whole visible wavelength range (Eg of Co-L was about 1.85 eV, as shown in Fig. S6†). At the same time, the optical response intensity of the Co-L/C3N4 hybrid material was significantly stronger than that of ordinary C3N4. With an increase in Co-L ligand content, the fluorescence intensity increased gradually, especially in the range of 550–650 nm. This phenomenon showed that the introduction of Co-L effectively improved the light absorption ability of the C3N4 material.63
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Fig. 5 (a) The UV-visible diffuse reflectance spectra of C3N4 and Co-L/C3N4; (b) the bandgap energy of C3N4 and Co-L/C3N4. |
As shown in Fig. S7,† the Mott–Schottky plot was obtained in aqueous solutions containing 0.1 M KCl at pH = 7.0 to estimate the EFB of Co-L and C3N4, respectively. The values of EFB were estimated to be −0.86 V and −0.97 (vs. NHE) for Co-L and C3N4, respectively. Compared with C3N4, a positive shift in the EFB of Co-L demonstrated a decrease in the bending of the band edge, thus facilitating electron transfer.64 The reason for the improvement in the photocatalytic activity of the Co-L/C3N4 nanocomposites was investigated by photochemical experiments. As shown in Fig. 6a, the photocurrent responses of C3N4 were much lower than that of Co-L combined C3N4 due to the rapid recombination of the photoexcited e− and h+. However, the photocurrent intensity increased dramatically along with the introduction of Co-L, and the Co-L/C3N4-15 catalyst exhibited the highest photocurrent density, which is consistent with the steady-state PL results. The obvious changes in the current response of the Co-L/C3N4 samples under irradiation indicated the good photo-harvesting capability of the prepared samples. Moreover, after several switching cycles, the photo-response was basically stable, further indicating the strong light corrosion resistance of the nanocomposites.65,66 At the same time, it was observed that the transient current between the lamps decreased, which may be caused by the accumulation of charges before the lamp is turned on. The photoelectric response was closely related to the content of Co ions. The photocurrent of Co-L/C3N4-15 was 3 times that of C3N4, which indicated the excellent photo-response of the composite nanomaterial. For nano-photocatalysts, reducing the interfacial resistance can promote charge transfer and thus improve photocatalytic performance.67 The interfacial properties of semiconductors are usually studied by electrochemical impedance spectroscopy (EIS).68 The interfacial resistance of the sample is expressed by the radius of the semicircle in the EIS.69 As shown in Fig. 6b, the radius of the C3N4 curve is larger than those of the Co-L loaded catalysts, and the radius of the semicircle decreases obviously after the introduction of Co ions, indicating that the addition of Co-L clearly reduces the resistance at the C3N4 interface. The interface of the Co-L/C3N4-15 composite nanomaterials had minimum resistance, which is consistent with the results of the photocurrent.
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Fig. 6 (a) Transient photocurrent response of C3N4 and Co-L/C3N4; (b) electrochemical impedance spectra of C3N4 and Co-L/C3N4. |
Fluorescence spectroscopy is an effective method to investigate the efficiency of photogenerated electron–hole separation in semiconductors.70 The fluorescence spectra of C3N4 and Co-L/C3N4 were measured at the same excitation wavelength (λex = 390 nm). As shown in Fig. 7a, C3N4 showed a strong fluorescence peak near 455 nm. After Co-L was loaded on C3N4, the fluorescence peak intensity of Co-L/C3N4 decreased significantly, indicating effectively suppressed recombination of the photogenerated charges. Furthermore, the photogenerated electron–hole recombination is also the critical factor to improving the photocatalytic oxidation efficiency. As shown in Fig. 7b, to further study the behaviour of the charge carriers in the samples, the time-resolved PL spectra were recorded, and the results are shown in Fig. 7b. C3N4 afforded a shorter average fluorescence lifetime (3.07 ps) compared with the Co-L/C3N4 (5.79 ps), which fully implied that the activated state in Co-L/C3N4 was long-lived than that in C3N4. The longer lifetime of electrons could be attributed to the remarkable separation of the photogenerated electron–hole pairs.71–73
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Fig. 7 (a) The PL spectra of C3N4 and different ratios of Co-L/C3N4. (b) The transient fluorescence spectra of C3N4 and Co-L/C3N4. |
The IR spectra of 4-hydroxybenzaldehyde and 4-hydroxyphenylglycolic acid in water were collected from a series of undersaturated solutions with known solute concentrations. To exhibit the reaction clearly, the differential absorption (ΔA) data was collected and processed, as shown in Fig. 8a. Peaks pointing down indicated bands disappearing, while those pointing up corresponded to new bands appearing due to the catalytic reaction. The increased intensity of the ΔA value at 1650 cm−1 was vested to the band of CO stretching vibration, which represents the generation of 4-hydroxybenzaldehyde by oxidation of benzyl alcohol in 4-hydroxyphenylglycolic acid.74 At the same time, the increased ΔA peaks at 1245 and 1170 cm−1 (as shown in Fig. 8b) belonged to the C–C stretching vibration and the conjugation of aromatic ketones following the 4-hydroxybenzaldehyde ketonic acid generation.75 The peaks at 1520 cm−1 and 1480 cm−1 were attributed to the intermediates of the conversion of 4-hydroxyphenylglycolic acid to ketonic acid. The peak at 1020 cm−1 was attributed to the C–C stretching vibration. The decline in the peaks was attributed to the probable fracture of C–C caused by the decarboxylation of the intermediate ketonic acid.76 UV-visible spectroscopy was an important method to study the oxidation of 4-hydroxymandelic acid to 4-hydroxybenzaldehyde. As shown in Fig. S8,† the decrease in the strong absorption peak at 249 nm could be attributed to the π–π* transition of the benzene ring. The absorption peak at 332 nm was attributed to the n–π* transition of the aldehyde oxygen atom. The changes in the UV-visible spectrum indicated the transformation of 4-hydroxymandelic acid to 4-hydroxybenzaldehyde clearly under irradiation.
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Fig. 8 (a) The 2D in situ FTIR spectra of 4-hydroxyphenylglycolic acid oxidation under irradiation. (b) The 3D in situ FTIR spectra of 4-hydroxyphenylglycolic acid oxidation under irradiation. |
On the basis of the above results, a plausible mechanism for the catalytical process has been proposed, as shown in Fig. 9. The Co-L loaded to C3N4 significantly enhances the visible light absorption, which has been proven by the UV-Vis and PL valence band spectra analysis. Therefore, under visible light irradiation, electrons are excited to the conduction band from the valence band of C3N4, with the holes staying on the valence band simultaneously.77–79 The electrons in the conduction band of Co-L/C3N4 can be trapped by electrophilic O2 to produce superoxide radical anions (˙O2−).80,81 On the other hand, the transition of Co2+/Co3+ ensures the generation of ˙O2−, which causes the substrate oxidation reaction. The high concentration of ˙O2− is captured by p-hydroxymandelic acid and further experiences the hydroxylation process to give OH− finally. The deprotonated p-hydroxymandelic acid forms the pivotal intermediate (α-keto carboxylate radical) to accomplish the oxidation process. Simultaneously, p-hydroxybenzaldehyde is generated following the decarboxylation of the pivotal intermediate. The continuously generated ˙O2− radicals greatly promote the conversion rate of p-hydroxymandelic acid in the photocatalytic process.
Footnote |
† Electronic supplementary information (ESI) available: The SEM, TEM and UV-visible DRS of Co(II)/C3N4, the HOMO and LUMO information of the mandelic acid derivatives. See DOI: 10.1039/d1ra08256f |
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