Sukanya Borthakurab,
Riya Dasa,
Purashri Basyachab,
Karanika Sonowalab and
Lakshi Saikia*ab
aAdvanced Materials Group, Materials Sciences and Technology Division, CSIR-North East Institute of Science and Technology, Jorhat 785006, Assam, India. E-mail: l.saikia@gmail.com; lakshi_saikia@yahoo.com; lsaikia@neist.res.in; Fax: +91 0376 2370011; Tel: +91 9957031635
bAcademy of Scientific and Innovative Research, Ghaziabad, UP 201002, India
First published on 3rd January 2024
Facile, cost-effective and eco-friendly synthesis of N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 photocatalysts towards efficient degradation of environmental pollutants was achieved. The as-synthesized 2 wt% N-doped ZnO@g-C3N4 and 2 wt% S-doped ZnO@g-C3N4 achieved 96.2% and 90.4% degradation efficiencies towards crystal violet (100 ppm) within 45 min irradiation and 99.3% and 92.3% photocatalytic degradation efficiencies towards brilliant green (100 ppm) dye within 30 min irradiation, respectively, under a normal 90 W LED light instead of an expensive commercial light source. Moreover, the N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites showed excellent stability in the photodegradation of crystal violet and brilliant green dyes. The modification made on ZnO by doping with nitrogen and sulphur enhances the visible-light absorption as well as the separation of photoexcited charge carriers. The active radicals ˙OH and ˙O2− are both identified to play important roles in the photodegradation of crystal violet and brilliant green.
Recently, semiconductor photocatalysis has attracted remarkable attention due to its clean and economic process for the complete degradation of organic contaminants. Among the semiconductors, ZnO is a promising material for advanced applications because of its unique features, including environmental stability, wide band gap, low cost, non-toxicity and unique chemical and physical properties.3,4 However, the wide band gap and low charge separation characteristic limit the photocatalytic activity of ZnO.5 To extend its response into visible light and improve its electron–hole separation efficiency, many attempts have been made, such as doping with metal and non-metal ions, controlling the morphology, forming a heterojunction with other materials.6,7 Among these, metal and non-metal doping have drawn much interest.8 Of the non-metal elements, N has proven to be a suitable p-dopant because the ionic radius and electronegativity of N are very close to those of O; hence, N doping may result in minimum strain in ZnO.9 Conversely, doping S is an efficient method for enhancing the visible-light activity of ZnO. Because of its large electronegativity as well as the size difference between S (r2− = 0.18 nm) and O (r2− = 0.14 nm), S-doping in ZnO helps to modulate the electrical and optical properties of ZnO.10 Therefore, both N- and S-doping can be considered potential pathways for extending the visible-light absorption of ZnO.
Graphitic carbon nitride (g-C3N4), a great potential material, has received significant interest because of its probable applications in environmental pollutant degradation, catalysing water splitting for H2 evolution, transesterification, hydrogen production, oxygen reduction and reducing carbon dioxide under visible-light irradiation due to its moderate band gap (2.7 eV), cost-effectiveness, unique electronic and optical properties, high stability and earth-abundant nature.11,12 However, the photocatalytic performance of this semiconductor photocatalyst is still limited because of its small specific surface area and fast recombination of charge carriers.12 This situation can be ameliorated through appropriate modification protocols, such as doping with organic or inorganic elements, coupling with other semiconductor components, and building heterostructures with another semiconductor.13 Constructing a suitable heterojunction composite by semiconductor coupling with a suitable band structure is an efficient way to improve the photo-excited charge separation.14 To date, various semiconductors have been investigated to construct g-C3N4 based composite photocatalysts such as ZnFe2O4/g-C3N4,15 WO3/g-C3N4,12 SnO2/g-C3N4,16 Fe2O3/g-C3N4,17 Ag3PO4/g-C3N4,18 ZnWO4/g-C3N4,19 SrTiO3/g-C3N4,20 CuCr2O4/g-C3N4,21 TiO2/g-C3N4,22 ZnO/g-C3N4,23 N–TiO2/g-C3N4,24 S–TiO2/g-C3N4,25 etc., to improve the visible-light-driven photocatalytic efficiency. Suneel et al. observed that N–ZnO/g-C3N4 nanocomposite was an efficient visible-light active photocatalytic material towards the degradation of toxic pollutants like rhodamine B, thiadiazol, nitrobenzene and tetracycline.13 Santosh et al. reported that core–shell nanoplates of N-doped ZnO/g-C3N4 showed improved photocatalytic activity towards the visible-light assisted degradation of rhodamine B.9 Xi-Yu et al. prepared a g-C3N4/S-doped ZnO nanocomposite via a one-pot method using sodium lignosulfonate which showed efficient photodegradation towards phenol and methylene blue.26
This article describes a facile eco-friendly synthesis strategy for N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites with remarkably improved visible-light induced catalytic efficiency. The photocatalysts were prepared by a simple cost-effective sonication-assisted route with different loadings of N-doped ZnO and S-doped ZnO nanoparticles. The excellent performance of N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites was assessed for the photodegradation of crystal violet and brilliant green dyes under 90 W LED light irradiation. The use of a 90 W LED light having a luminous intensity of 8060 candela instead of any commercially available expensive, high intensity light source for photocatalytic degradation represents an energetically economical alternative. The extended adsorption in the visible-light region and the higher separation efficiency of photo-excited charge carriers promoted the photocatalytic activity under visible-light irradiation.
The XRD patterns of g-C3N4 and 2 NZCN and 2 SZCN nanocomposites are depicted in Fig. 1. The strong peak at 2θ = 27.18 corresponds to the (002) crystal phase, which is a characteristic interplanar stacking structure of graphitic material (JCPDS-87-1526, inset Fig. 1).15 In the case of N-doped ZnO and S-doped ZnO nanoparticles, the characteristic peaks correspond to the hexagonal wurtzite phase of ZnO without any impurity, suggesting that the crystal structures remain the same after the incorporation of nitrogen and sulphur, respectively (JCPDS-36-1451).26,27 The diffraction patterns of N-doped ZnO and S-doped ZnO are significantly broader than that of bare ZnO due to their decreasing crystallinity because of the introduction of N and S into the ZnO lattice. The XRD patterns show no extra diffraction peaks, indicating N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 to be two-phase nanocomposite hybrids.
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Fig. 1 XRD patterns of 2 NZCN and 2 SZCN nanocomposites and g-C3N4. Inset: XRD patterns of N-doped ZnO and S-doped ZnO nanoparticles. |
The FT-IR spectra of pure g-C3N4, pure ZnO, N-doped ZnO, S-doped ZnO, and 2 NZCN and 2 SZCN nanocomposites are depicted in Fig. S1.† In the cases of ZnO, N-doped ZnO and S-doped ZnO, the peaks at 400–550 cm−1 correspond to the Zn–O stretching vibration.26,27 As shown in Fig. S1,† the IR absorption bands showed the typical molecular structure of pure g-C3N4. A broad peak centered at 3152 cm−1 corresponds to the N–H stretching vibration and the peak at 808 cm−1 is assigned to the stretching vibrational mode of the s-triazine ring of g-C3N4.15 The peaks ascribed to the stretching vibrations of the CN heterocycles are within the range of 1200–1650 cm−1 for the pure g-C3N4 nanosheets. It is observed that all the major characteristic peaks of g-C3N4, N-doped ZnO and S-doped ZnO are retained in the FT-IR spectra of 2 NZCN and 2 SZCN nanocomposites. From the figure, it was seen that, in the cases of 2 NZCN and 2 SZCN, the major distinctive bands of g-C3N4 are retained in the nanocomposites, which indicates that the structural features of g-C3N4 are retained after the hybridization process. Furthermore, the main characteristic peaks of g-C3N4 in the 2 NZCN and 2 SZCN nanocomposites slightly shift to higher wave numbers, which is attributable to the extended conjugated system in the nanocomposites.27
TGA was carried out from room temperature to 800 °C at a heating rate of 10 °C min−1 under N2 flow in order to calculate the contents of N-doped TiO2 and S-doped TiO2 nanoparticles on the g-C3N4 nanosheets in the as-synthesized N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites. The TG/DTA plots of as-prepared pure g-C3N4 and N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites are depicted in Fig. S2.† For bare g-C3N4, a weight loss occurred from 500 °C to 700 °C due to the decomposition or condensation of g-C3N4.28 For the N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites, the stability of the nanocomposites significantly decreased due to the oxidation and decomposition of g-C3N4 in the composite materials.30 The thermal stability decreased from 482 °C to 694 °C and from 485 °C to 698 °C for the N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites, respectively, compared to g-C3N4, indicating the close contact between N-doped ZnO and S-doped ZnO with the g-C3N4 nanosheets. The residual weight fractions of the 2 NZCN and 2 SZCN nanocomposites were found to be 1.3% and 2.6%, respectively, and these are considered to be the contents of N-doped ZnO and S-doped ZnO in the 2 NZCN and 2 SZCN nanocomposites, respectively.
UV-vis diffuse reflectance spectroscopy (DRS) was carried out to investigate the visible-light absorption of the N-doped ZnO@ g-C3N4 and S-doped ZnO@g-C3N4 nanocomposite photocatalysts. The absorption edge of pure g-C3N4 is around 452 nm (Fig. 2(a)). The absorption of N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 photocatalysts in the visible-light region is considerably enhanced and a red shift compared to bare g-C3N4 appeared due to the interaction of the g-C3N4 nanosheets with the N-doped ZnO and S-doped ZnO NPs in the nanocomposites.26 The wider light absorption region of the as-prepared nanocomposites is able to effectively produce more photo-generated charge carriers for better photocatalytic activity under visible-light absorption.30
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Fig. 2 (a) UV-vis spectra and (b) band gap energies of g-C3N4, N-doped ZnO, S-doped ZnO, and 2 NZCN and 2 SZCN nanocomposites. |
The band gap energy of samples was evaluated according to eqn (1),
αhυ = A (hυ − Eg)n/2 | (1) |
The Brunauer–Emmett–Teller (BET) specific surface areas of the photocatalysts were evaluated by their N2 adsorption–desorption isotherms (Fig. S3(a)–(c)†). The BET specific surface area of pure g-C3N4 and N-doped ZnO and S-doped ZnO nanoparticles were obtained as 66.5 m2 g−1, 147.9 m2 g−1 and 117.4 m2 g−1, respectively. The specific surface areas of the 2 NZCN and 2 SZCN nanocomposites are 89 m2 g−1 and 84 m2 g−1, respectively, which are lower than those of the pure N-doped ZnO and S-doped ZnO nanoparticles due to filling the interparticle space of the parent g-C3N4 photocatalyst with N-doped ZnO and S-doped ZnO NPs, respectively (Fig. S4(a) and (b)†). Table S1† summarizes the BET surface areas of the as-synthesized N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites with different contents of N-doped ZnO and S-doped ZnO nanoparticles, respectively. As can be seen, with an increase in the contents of N-doped ZnO and S-doped ZnO nanoparticles, there is a gradual decrease in the specific surface area values in the nanocomposites. Low contents of N-doped ZnO and S-doped ZnO NPs with larger surface areas results in lower catalytic efficiencies than those of the 2 NZCN and 2 SZCN nanocomposites, as they can produce few electron–hole pairs for the photocatalytic process. However, with an increase in the content of N-doped ZnO and S-doped ZnO up to 6 wt%, the catalytic activity deceases because the low surface area restricts the contact between pollutant and photocatalyst. A morphological evaluation of the as-synthesized photocatalysts was conducted by FESEM, TEM and HRTEM analysis. Fig. 3(a)–(c) show the FESEM images of bare g-C3N4 and N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites. As depicted in Fig. 3(a), bare g-C3N4 consists of lamellar shaped 2D nanosheets with a smooth surface. In Fig. 3(b) and (c), g-C3N4 retains its flat layer structure even after the loading of N-doped ZnO and S-doped ZnO nanoparticles, respectively.
The small, aggregated structures of the N-doped ZnO and S-doped ZnO nanoparticles are clearly embedded over the g-C3N4 nanosheets and thus lead to the construction of 2D–2D nanocomposites between g-C3N4 and the N-doped ZnO and S-doped ZnO nanoparticles (Fig. 4(b) and (c)).
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Fig. 4 TEM images of (a) g-C3N4, (b) 2 NZCN, and (c) 2 SZCN. (d) HRTEM image of 2 NZCN nanocomposite. |
To investigate the microstructure and morphology of the photocatalysts, TEM and HRTEM were performed. As shown in Fig. 4(a), bare g-C3N4 exhibits planar, thin, stacked layers and an irregular sheet-like morphology. In Fig. 4(d), the lattice plane of 0.24 nm corresponds to the (101) diffraction plane of ZnO and the lattice plane of 0.32 nm corresponds to the characteristic (002) plane of g-C3N4 in the N-doped ZnO@g-C3N4 nanocomposite. Therefore, the interfacial contact of the N-doped ZnO (101) with the g-C3N4 (002) lattice plane inhibits the recombination probability, hence improving the catalytic activity.13
The EDX elemental mapping analysis clearly reveals the presence of the constituent elements (C, N, O and Zn) in the 2 wt% N-doped ZnO@g-C3N4 nanocomposite, as depicted in Fig. S5.† Similarly, the EDX elemental mapping analysis of the 2 wt% S-doped ZnO@g-C3N4 nanocomposite indicates the presence of C, N, O, Zn and S elements, as depicted in Fig. S6.†
XPS analysis was performed in order to explicate the surface chemical composition and the chemical state of the photocatalyst. As depicted in Fig. 5(a) and 6(a), the survey XPS of N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites reveal the presence of C 1s, N 1s, O 1s, and Zn 2p elements and C 1s, N 1s, O 1s, Zn 2p, and S 2p elements, respectively. Regarding C 1s in Fig. 5(b) and 6(b), the three major peaks at 283.79 eV, 287.08 eV and 288.65 eV in 2 NZCN and the peaks at 284.05 eV, 286.17 eV and 287.08 eV in the 2 SZCN nanocomposite are associated with sp2 C–C bonds, sp3 coordinated carbon species from the defects on the g-C3N4 surface and C–N–C coordination, respectively.29,31 The high-resolution spectra of N 1s display three peaks at binding energies of 397.59 eV, 398.50 eV and 399.69 eV in the 2 NZCN nanocomposite and 397.62 eV, 399.01 eV and 400.06 eV in the 2 SZCN nanocomposite (Fig. 5(c) and 6(c)). The binding energies at 397.59 eV and 397.62 eV may be attributed to sp2 bonded carbon in nitrogen-containing aromatic rings (CN–C) and the two peaks at 399.69 eV and 399.01 eV and the one at 400.06 originate from N-(C)3 units and the N atom in amino moieties, respectively.31,32 In the N 1s spectrum of 2 NZCN nanocomposite, the N 1s peak at 398.50 eV corresponds to the Zn–N nitrogen, which clearly shows the successful doping of N at the O sites of ZnO.8 In Fig. 5(d) and 6(d), the high-resolution spectrum of O 1s can be dissociated into two major peaks at 530.92 eV and 532.34 eV for the 2 NZCN nanocomposite and at 531.49 eV and 532.32 eV for the 2 SZCN nanocomposite, corresponding to the lattice oxygen of ZnO and absorbed water on the catalyst surface, respectively.26 Peaks at 1020.79 eV and 1044 eV and 1021.15 eV and 1044.43 eV are observed in the high-resolution spectra of Zn 2p in 2 NZCN and 2 SZCN nanocomposites, respectively (Fig. 5(e) and 6(e)), and correspond to Zn 2p3/2 and Zn 2p1/2, respectively.26,29 As shown in Fig. 6(f), the high-resolution spectrum of S 2p could be dissociated into two major peaks at 160.99 eV and 167.08 eV, ascribed to the C–S bond and sulphur oxide powder during calcination process, respectively, which evidences the successful doping of S into the crystalline ZnO substrate.26,33
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Fig. 5 (a) XPS survey spectrum, (b) C 1s XPS spectrum, (c) N 1s XPS spectrum, (d) O 1s XPS spectrum and (e) Zn 2p XPS spectrum of 2 NZCN nanocomposite. |
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Fig. 6 (a) XPS survey spectrum, (b) C 1s XPS spectrum, (c) N 1s XPS spectrum, (d) O 1s XPS spectrum, (e) Zn 2p XPS spectrum and (f) S 2p XPS spectrum of 2 SZCN nanocomposite. |
The room temperature PL spectra of the as-synthesized catalysts were studied to evaluate the separation and recombination probability of charge carriers in g-C3N4 and the N-doped ZnO and S-doped ZnO nanoparticles at 325 nm (Fig. 7). As depicted in Fig. 7, the bare g-C3N4 has a major emission peak centered at about 425 nm indicating the band–band PL phenomenon.34 Remarkably, the PL emission intensity becomes weaker for the N-doped ZnO@ g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites with the addition of the N-doped ZnO and S-doped ZnO nanoparticles, respectively, to the g-C3N4 nanosheets. The PL emission intensity increases due to the recombination probability of charge carriers, and the decrease in the emission intensity indicates the suppressed recombination of charge carriers.35 Therefore, N-doped ZnO@ g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites more effectively inhibit the recombination of photo-excited charge carriers for better photocatalytic activity.
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Fig. 7 Photoluminescence spectra of g-C3N4, N-doped ZnO, S-doped ZnO, and 2 NZCN and 2 SZCN nanocomposites. |
The photocatalytic activities of N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites were evaluated in terms of the visible-light assisted degradation of two dye molecules, namely crystal violet (CV) and brilliant green (BG). UV-vis analysis visibly indicates the changes in the molecular structures of CV and BG in visible-light-driven photodegradation using the 2 NZCN and 2 SZCN photocatalysts. The characteristic absorption bands of CV and BG, located at 590 and 625 nm, respectively,36,37 decrease rapidly as the irradiation time increases and nearly vanish after 30 min and 45 min of visible-light assisted irradiation by the 2 NZCN and 2 SZCN photocatalysts, respectively. As depicted in Fig. 8(a)–(d), the discolorations of CV and BG, respectively, follow the order Cat/H2O2/vis > Cat/vis > Cat/H2O2 > Cat > H2O2/vis > H2O2. In the blank experiment, the direct photolysis of CV and BG is almost negligible without the photocatalyst, indicating that the degradation of CV and BG arises from the photocatalytic reaction instead of photolysis. The discoloration due to the photocatalyst hardly occurred in the absence of H2O2 and visible light, suggesting that the photocatalyst did not lead to significant adsorption of the dyes. In the presence of the catalyst, visible light and H2O2, the discoloration of dye was significantly enhanced, suggesting the crucial role of the as-synthesized N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites towards the efficient degradation of both CV and BG dyes. The as-synthesized 2 NZCN nanocomposite exhibits the highest catalytic efficiency towards degradation of the dyes, i.e. 96.2% of CV is degraded within 45 min and 99.3% of BG is degraded within 30 min of H2O2 assisted visible-light irradiation by 2 NZCN photocatalyst. Similarly, in the presence of both visible light and H2O2, the as-prepared 2 SZCN photocatalyst exhibits 90.4% CV degradation and 92.3% BG degradation.
The consumption and decomposition of H2O2 in the photocatalytic degradation of CV and BG by the as-synthesized 2 NZCN and 2 SZCN photocatalysts under various conditions were evaluated by a simple and fast spectrophotometric metavanadate assisted method38 and followed the order Cat/H2O2/vis > Cat/H2O2 > H2O2/vis > H2O2. As seen in Fig. S7(a) and (c),† it was observed that, in the presence of 2 NZCN photocatalyst and visible light, the highest consumption of H2O2 was observed as 97% and 96.6% for CV and BG degradations, respectively. Similarly, in H2O2 assisted CV and BG degradation by 2 SZCN photocatalyst, the consumption of H2O2 was found to be 96.4% and 97.3%, as shown in Fig. S7(b) and (d),† respectively.
The photocatalytic efficiencies of the as-prepared N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites were examined in the visible-light assisted photodegradation of CV and BG. The catalytic efficiencies of the N-doped ZnO and S-doped ZnO are higher compared to that of bare ZnO, which clearly signifies that the N- and S-doping considerably enhance the spectral response to the visible region (Fig. 9(a), (c) and (b), (d)). The g-C3N4, pure N-doped ZnO and pure S-doped ZnO show low photocatalytic degradation efficiencies of almost 55.6%, 32.6% and 23.6%, respectively, in the photocatalytic degradation of CV. Similarly, the photocatalytic efficiencies of g-C3N4, pure N-doped ZnO and pure S-doped ZnO are found to be 64.2%, 40.2% and 28.3%, respectively, for the degradation of BG. After being combined with g-C3N4, the catalytic efficiencies of N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites improved significantly and the weight percentages of pure N-doped ZnO and S-doped ZnO have significant influence on the degradation efficiencies. The catalysts with 2 wt% N-doped ZnO and 2 wt% S-doped ZnO loading exhibit the best photocatalytic performance in dye degradation, resulting in visible-light induced photocatalytic activities of 96.2% and 90.4% within 45 min for CV degradation and 99.3% and 92.3% within 30 min for BG degradation, respectively. The ICP-MS analysis indicated that the Zn contents in 2 NZCN and 2 SZCN were found to be 9.0 ppm and 13.37 ppm, respectively. Similarly, the catalyst turnover numbers (TON) for the 2 NZCN supported photocatalytic degradations of BG and CV were calculated on the basis of Zn content to be 1.7 × 104 and 1.1 × 104, respectively. Accordingly, for the 2 SZCN catalyzed photocatalytic degradation of BG and CV, the catalyst turnover numbers (TON) were found to be 1.1 × 104 and 6.7 × 103, respectively, based on Zn content, indicating higher catalytic activity towards efficient degradation. Therefore, developing novel catalysts for reactions with high TONs is advantageous for practical applications.39
The reaction processes of CV and BG photodegradation over g-C3N4, pure N-doped ZnO and pure S-doped ZnO with different loadings of N-doped ZnO and S-doped ZnO successfully follow the pseudo-first-order chemical kinetic model in eqn (2).
ln(C/C0) = −kt | (2) |
In this equation, k represents the first-order rate constant (min−1), C0 is the initial concentrations of CV and BG and C represents the concentrations at reaction time t. The k values of all the photocatalysts for CV and BG degradation were calculated and are depicted in the insets of Fig. 9(a), (c) and (b), (d), respectively. The as-synthesized 2% N-doped ZnO@g-C3N4 and 2% S-doped ZnO@g-C3N4 nanocomposites exhibited rate constants of 0.05 min−1 and 0.04 min−1 for CV and 0.16 and 0.08 for BG, respectively. The rate constants of 2 NZCN are 2.5 and 5 times higher than those of g-C3N4 and N-doped ZnO nanoparticles, respectively, in the case of CV. Similarly, the rate constants of 2 SZCN are 2 and 6.6 times higher than those of g-C3N4 and S-doped ZnO nanoparticles, respectively, in the case of CV. A significant enhancement of the photocatalytic efficiency of 2 NZCN nanocomposite towards the degradation of BG was seen, at 5.3 and 16 times higher than those of g-C3N4 and N-doped ZnO nanoparticles, respectively. For the photodegradation of BG, the optimal catalytic efficiency of 2 SZCN nanocomposite is 2.6 and 8 times higher than those of g-C3N4 and S-doped ZnO nanoparticles, respectively. However, with further increases in the contents of N-doped ZnO and S-doped ZnO for the N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites, the degradation efficiencies decrease due to the excessive amount of N-doped ZnO and S-doped ZnO on the g-C3N4 surface leading to the reduction of heterojunctions between the g-C3N4 and the N-doped ZnO and S-doped ZnO. Furthermore, the number of active sites on g-C3N4 was reduced, which is necessary to quench the holes due to the excessive amounts of N-doped ZnO and S-doped ZnO.40
The role of initial H2O2 concentration on the visible-light assisted degradation efficiencies for CV and BG can be considered a major factor. In the case of photocatalytic degradation of CV by the 2 NZCN and 2 SZCN nanocomposites, it was observed that, with increasing initial H2O2 concentration from 0.005 M to 0.10 M, the pseudo first order kinetic constant (k) increased gradually from 0.01 to 0.05 and 0.02 to 0.04, respectively, and was then saturated beyond 0.01 M (Fig. S8(a) and (b)†). Similarly, the rate constant value enhanced considerably from 0.02 to 0.16 and 0.03 to 0.08 in the concentration range 0.005 M to 0.10 M for the degradation of BG by 2 NZCN and 2 SZCN nanocomposites, respectively, as shown in Fig. S9(a) and (b).† This result shows that only a small amount of H2O2 is required to efficiently run the photocatalytic reactions. The excessive amount of H2O2 essentially acts as a self-scavenger for ˙OH according to eqn (3) and (4).41
H2O2 + ˙OH → ˙OOH + H2O | (3) |
˙OOH + ˙OH → H2O + O2 | (4) |
The pH effect may be considered one of the most impactful parameters. The influence of pH on the catalytic process for both CV and BG by our as-synthesized 2 NZCN and 2 SZCN photocatalysts is illustrated in Fig. S10(a)–(d),† respectively. The effects of initial pH on the photodegradation of both CV and BG were investigated by changing the pH of the dye solution from 2 to 11, keeping the catalyst dose (200 mg L−1) and concentration of dye (100 ppm) constant. The pH of the suspension was varied by adding the proper quantity of NaOH or HCl. The photocatalytic degradation rates of both cationic dyes CV and BG increase with a gradual increase in pH value and finally achieve the maximum rate at pH = 9. Thereafter, further enhancement of the pH leads to a decrease in catalytic activity because the higher pH leads the semiconductor surface to become negatively charged, which is favourable for better adsorption of the cationic dye molecule onto the catalyst surface.42 Also, a higher pH value leads to the production of more of active species ˙OH due to the interaction between the photo-excited holes (h+) of the catalyst and the OH− of the base.43 This type of close interaction of the adsorbed dye molecule with ˙OH radicals subsequently causes the higher rate of catalytic activity. However, at pH > 9, the cationic dye changes into a neutral molecule, thereby making adsorption onto the photocatalyst surface difficult and resulting in a decrease in degradation efficiency.
The stability and recyclability of photocatalysts are considered very important factors in photocatalytic reactions. To evaluate the stability and recyclability of the as-synthesized 2 NZCN and 2 SZCN nanocomposites, seven successive photocatalytic experimental runs were carried out with the addition of recycled 2 NZCN and 2 SZCN nanocomposites to fresh CV and BG solutions at the same concentration of the catalyst under visible-light irradiation. Prior to the reusability experiments, the catalyst was filtered and dried at 100 °C. The catalytic activity of 2 NZCN nanocomposite for the degradation of CV and BG remains almost consistent, decreasing only from 96.2% to 92.6% in the case of CV and from 99.3% to 95.8% in the case of BG even after seven successive runs, indicating the good recyclability of the photocatalyst (Fig. 10(a) and (c)). Similarly, the photocatalytic activity of 2 SZCN nanocomposite was retained, from 90.4% to 86.9% (in the case of CV solution) and from 92.3% to 88.3% (in the case of BG solution) after the seventh catalytic cycle, indicating the photostability of the catalysts for potential applications (Fig. 10(b) and (d)). Therefore, N-doped ZnO@g-C3N4 and S-doped ZnO@gC3N4 nanocomposites act as stable photocatalytic materials towards environmental protection. Furthermore, there is no obvious difference in the SEM images of 2 NZCN and 2 SZCN nanocomposites, as depicted in Fig. S11(a) and (b),† respectively, after the seventh catalytic cycle. XPS analysis of the recovered 2 NZCN and 2 SZCN photocatalysts (Fig. S12 and S13†) indicates their high chemical stability in the photodegradation process. Therefore, N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites act as stable photocatalytic materials towards environmental protection.
To investigate the photocatalytic degradation mechanism, various scavengers were employed to investigate the major oxidative species involved in the photodegradation reaction. Here, isopropyl alcohol, ascorbic acid and EDTA were utilized as ˙OH scavenger, ˙O2− scavenger and h+ scavenger, respectively, while potassium iodide was applied to reduce both ˙OH and h+ radical. Fig. 11(a) and (c) depict the photocatalytic efficiencies of 2 NZCN nanocomposite with CV and BG, respectively, in the presence of various scavengers. When IPA was added into the reaction mixture, the photocatalytic efficiencies were significantly reduced to 37.2% and 39.6%, respectively, indicating the major role of ˙OH radical in the degradation mechanism of CV and BG by 2 NZCN photocatalyst. Similarly, after the addition of ascorbic acid, the photocatalytic efficiencies are reduced to 42.4% and 43.2% for CV and BG, as depicted in Fig. 11(a) and (c), respectively, indicating the major role of the ˙O2− radical in the photocatalytic process. However, the photocatalytic efficiencies were almost unvarying with the addition of EDTA, suggesting the hole is not the major active species. For the 2 SZCN photocatalyst, upon the addition of IPA, the conversion percentages of CV and BG were greatly decreased to 34.2% and 43.2%, respectively. Similarly, the addition of ascorbic acid decreases the photocatalytic efficiencies of both CV and BG to 39.6% and 48.6%, respectively (Fig. 11(b) and (d)). The addition of EDTA led to non-significant changes, indicating that h+ plays a negligible role in the photodegradation of CV and BG over both the 2 NZCN and 2 SZCN photocatalysts.
The positions of the valence band and conduction band of the as-synthesized photocatalysts could be found by using eqn (5) and (6).44
EVB = χ − Ee + 0.5Ebg | (5) |
ECB = EVB − Ebg | (6) |
In the above equations, EVB, ECB, χ, Ee and Ebg denote the valence band edge potential, the conduction band edge potential, the electronegativity of the semiconductor, the energy of the free electrons on the hydrogen scale, i.e. 4.5, and the band gap energies of g-C3N4, N-doped ZnO and S-doped ZnO, i.e. 2.77 eV, 2.99 eV and 3.05 eV, respectively. Hence, the ECB values of g-C3N4, N-doped ZnO and S-doped ZnO are obtained as −1.24 eV, −0.20 eV and −0.23 eV, respectively. The EVB values of g-C3N4, N-doped ZnO and S-doped ZnO are determined to be 1.53 eV, 2.79 eV and 2.82 eV, respectively.
Generally, semiconductor-based photocatalytic reactions are initiated by the generation of some photo-excited charge carriers. A plausible mechanism for the visible-light assisted photocatalytic degradation of both CV and BG by the as-synthesized N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites is illustrated in Fig. 12(a) and (b), respectively. In the presence of a visible-light source, the movement of photo-excited charge carriers in g-C3N4, N-doped ZnO and S-doped ZnO from the VB to the CB separate the photo-generated charge carriers on the photocatalyst surface. The photo-excited electrons could easily migrate from the CB of g-C3N4 to the CB of N-doped ZnO and S-doped ZnO, as the CB level of g-C3N4 is more negative than those of N-doped ZnO and S-doped ZnO, thereby enhancing the separation of the photo-excited charge carriers.9 In both N-doped ZnO and S-doped ZnO, the photo-generated electron in the CB can react with dissolved O2 to produce more active radicals which promote the dye degradation.45 The photo-induced electrons lead to the formation of more active radical superoxide anions (˙O2−) for the photocatalytic process. However, the majority of photo-excited holes on the VB of N-doped ZnO migrated to the VB of g-C3N4, as the VB potential of g-C3N4 (+1.4 eV NHE) is less positive than the standard redox potential E0 (H2O/˙OH) (+2.4 eV vs. NHE).46 Hence, the photo-excited holes can lead to the formation of ˙OH radicals for complete mineralization of the organic dye molecules.45 However, these ˙OH radicals can also be trapped using salicylic acid as a trapping agent.47 Compared with the individual components, the formation of N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 heterojunctions induces higher photocatalytic activity towards the degradation of organic pollutants.
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Fig. 12 Proposed mechanism for the photodegradation of CV and BG by (a) N-doped ZnO@g-C3N4 nanocomposite and (b) S-doped ZnO@g-C3N4 nanocomposite under visible-light irradiation. |
A comparison of some previously reported catalysts with the present catalysts towards the degradation of both crystal violet and brilliant green dyes is summarized in Table S2.†
Typically, 20 g of urea was placed in a well-closed silica crucible and heated at 4 °C min−1 to 550 °C for 2 h in a muffle furnace. The as-synthesized g-C3N4 was collected and ground into powder. The g-C3N4 nanosheets were synthesized by exfoliating the bulk g-C3N4 in deionized water. 200 mg of the obtained g-C3N4 was dispersed in 100 mL of distilled water, followed by ultrasonication and centrifugation at 15000 rpm.
In a typical process, zinc acetate dihydrate (0.10 mol) was put into 30 mL of distilled water and the suspension was stirred for 30 min in order to get a clear solution, followed by heating above 100 °C to get our desired pure ZnO nanoparticles.27
N-doped ZnO nanoparticles were prepared based on the previously reported method with a little modification.27 In a typical synthesis, zinc acetate dihydrate was mixed thoroughly with urea (molar ratio 1:
2) using a mortar and pestle, followed by adding 20 mL of distilled water. The colourless solution of zinc acetate urea complex was stirred, followed by heating at 100 °C in order to evaporate the water. The as-synthesized pale yellow coloured gel was washed, dried at 70 °C for 48 h and heated at 500 °C for 3 h to get N-doped ZnO nanoparticles.
The S-doped ZnO nanoparticles were prepared according to the following procedure. Typically, zinc acetate dihydrate and sulphur powder were mixed at a molar ratio of 1:
2. The resulting mixture was ultrasonically dispersed in 200 mL of water for 1 h in order to get a yellowish coloured solution. The suspension was dried using a Rotavapor followed by oven drying at 100 °C overnight. The dried product was calcined at 500 °C for 3 h in a muffle furnace.
An appropriate quantity of g-C3N4 was exfoliated in 100 mL of distilled water for 30 min. Different amounts of as-synthesized N-doped ZnO (1, 2, 4 and 6 mg) or S-doped ZnO (1, 2, 4 and 6 mg) were added into the suspension and ultrasonicated overnight. In order to get the desired N-doped ZnO@g-C3N4 and S-doped ZnO@g-C3N4 nanocomposites, water was removed with the help of a Rotavapor, followed by oven drying at 100 °C for 1 h. To investigate the effect of the loadings of N-doped ZnO and S-doped ZnO in the photocatalytic study, the corresponding samples of N-doped ZnO@g-C3N4 (1, 2, 4 and 6 wt%) and S-doped ZnO@g-C3N4 (1, 2, 4 and 6 wt%) nanocomposites were labelled as 1 NZCN, 2 NZCN, 4 NZCN, and 6 NZCN and 1 SZCN, 2 SZCN, 4 SZCN, and 6 SZCN, respectively. The dopant concentrations of N and S for the N-doped ZnO-g-C3N4 and S-doped ZnO-g-C3N4 nanocomposites were found to be 0.6 gm mL−1 and 0.06 gm mL−1, respectively.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3ra06488c |
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