Lan Anh
Luu Thi
a,
Quoc Tung
Trieu
a,
Thi Hue
Trinh
b,
Tuyet Mai
Nguyen Thi
c,
Cong Tu
Nguyen
a,
Tran Thanh
Tung
d and
Nguyen Xuan
Sang
*ef
aFaculty Engineering of Physics, Hanoi University of Science and Technology, No. 1, Dai Co Viet Street, Hai Ba Trung District, 100000 Hanoi, Vietnam
bFaculty of Electronics and Telecommunications, Electric Power University, No. 235 Hoang Quoc Viet Street, Hanoi, Vietnam
cSchool of Chemistry and Life Sciences, Hanoi University of Science and Technology, No. 1, Dai Co Viet Street, Hai Ba Trung District, 100000 Hanoi, Vietnam
dThe University of Adelaide, School of Chemical Engineering, Adelaide, SA 5005, Australia
eAtomic Molecular and Optical Physics Research Group, Institute for Advanced Study in Technology, Ton Duc Thang University, Ho Chi Minh City, Vietnam. E-mail: nguyenxuansang@tdtu.edu.vn
fFaculty of Electrical and Electronics Engineering, Ton Duc Thang University, Ho Chi Minh City, Vietnam
First published on 10th July 2025
This work presents an eco-friendly method for the preparation of a silver nanoparticle (AgNP) decorated g-C3N4 nanocomposite using purple leaf extract as a green reduction agent. The photocatalytic performance of the resulting nanocomposite was studied through the degradation of rhodamine B (RhB) dye pollution in an aqueous solution. X-ray diffraction analysis of powder samples revealed the coexistence of face-centered cubic AgNP crystalline and g-C3N4 structures, with a slight shift in the dominant diffraction peak (002) of g-C3N4, indicating successful incorporation of AgNPs. Optical analysis showed a reduction in the bandgap of the nanocomposite compared with that of the pure g-C3N4 sample. The photocatalytic ability of the nanocomposites was tested through the degradation of RhB dye, which was significantly enhanced by the presence of AgNPs, achieving a maximum degradation efficiency of approximately 95.3% after only 75 minutes of irradiation using the Ag@g-C3N4 nanocomposite with 7 wt% AgNPs as a photocatalyst. This enhancement is attributed to the efficient charge carrier separation and suppressed recombination rate at the photocatalyst interfaces.
Various methods, including increasing the surface area, reducing the electron–hole recombination rate and extending the visible light absorption region to longer wavelengths, are among the studies that have been carried out to improve the photocatalytic activity of g-C3N4. One of the effective solutions to separate the electron–hole pairs and prevent their recombination is to create composite materials using g-C3N4 and other metal nanoparticles. This hybridization significantly reduces electron–hole recombination as noble metal nanoparticles can serve as efficient electron acceptors due to their strong surface plasmon resonance effect.19,20 To enhance the photocatalytic activity, other semiconductor oxides such as TiO2 can also be modified with Ag to reduce contaminants in an aqueous phase.21 The doping, hybridization, modification or compositing of Ag with g-C3N4 may change the conductivity of the composite material compared to that of pure g-C3N4 due to the reduction of the energy barrier for the transfer of electrons. Pham et al. reported the fabrication of Ag/g-C3N4 material via a photoreduction method. The 20% Ag/g-C3N4 sample provides the highest photocatalytic efficiency of NO decomposition and reaches 80% under visible light irradiation.22 Dong Liang et al. prepared Ag/g-C3N4 for which the g-C3N4 was synthesized by urea pyrolysis at 550 °C with a heating rate of 15 °C min−1 for 3 h. The obtained results showed that the photocatalytic nitration of pharmaceutical intermediate halo-nitro-phenol, using various bromophenols and nitrites as raw materials, was significantly improved when using Ag/g-C3N4 composite as the photocatalyst compared with pure g-C3N4.23 In another work, the Ag/g-C3N4 composite was synthesized via polymerization and the silver mirror reaction. In the sample surveys, the sample containing 5% Ag had the highest hydrogen production rate which was 39 times higher than that of bulk g-C3N4 with a value of 568.9 μmol g−1 h−1.24 Hai Zhu et al. used an ultrasound-assisted method to prepare Ag/g-C3N4 catalysts for photocatalytic water splitting. The results showed that the optimal synthesis conditions were 60 W ultrasonic power for 35 s (residence time). The sample showing the best photocatalytic activity for the water splitting reaction was the 7 wt% Ag/g-C3N4 sample, which had a reaction rate constant 2.76 times higher than that of pristine g-C3N4.25
In this study, Ag was selected to investigate its interaction with g-C3N4 and its influence on the structural, physical and chemical properties and photocatalytic ability of g-C3N4. The photocatalytic activity was examined through the degradation of RhB dye. In addition, the effects of reaction parameters on the photocatalytic performance and the photocatalytic enhancement mechanism were systematically evaluated.
For the synthesis of Ag@g-C3N4 nanocomposites, predetermined amounts of AgNO3 and g-C3N4 were dissolved into 50 ml of purple leaf extract under the effect of magnetic stirring for about 60 minutes to obtain 50 ml of precursor suspension solution. This solution was transferred to a 100 ml hydrothermal autoclave. The hydrothermal reaction was performed at 80 °C for 24 h. The suspension obtained after the reaction was washed several times with distilled water to remove the by-products, and the samples were dried at 80 °C for 24 h. The experimental scheme is illustrated in Scheme 1. The Ag@g-C3N4 nanocomposites were designated according to their Ag contents as summarized in Table 1. The obtained samples are denoted as g-C3N4, ACN03, ACN07, ACN10 and ACN20, respectively, corresponding to the Ag contents in the synthesized samples of 3, 7, 10, and 20 weight percentage.
Sample name | Weight percent of Ag (wt%) | Weight of g-C3N4 (g) | Weight of Ag (g) |
---|---|---|---|
g-C3N4 | 0 | 0.300 | 0.000 |
ACN03 | 3 | 0.291 | 0.009 |
ACN07 | 7 | 0.279 | 0.021 |
ACN10 | 10 | 0.270 | 0.030 |
ACN20 | 20 | 0.240 | 0.060 |
Furthermore, the characteristic diffraction peak position (002) of the g-C3N4 nanocomposite samples was observed to gradually shift slightly toward lower 2θ values when the amount of Ag increased. This may indicate the influence of Ag nanoparticles on the crystal structure of g-C3N4, potentially due to lattice distortion or interfacial interactions.
The vibrations of the organic functional groups in ACN nanocomposite samples were studied using FTIR spectroscopy, as shown in Fig. 1b. The absorption peaks observed at wavenumbers 1640, 1564, 1413, 1326, and 1247 cm−1 are attributed to the typical stretching vibrations of CN heterojunctions.26,29 The vibration modes at wavenumbers 810 and 3169 cm−1 are due to the stretching vibrations of the triazine units and –NH, respectively. The wavenumber range from 3600 cm−1 to 3000 cm−1 corresponds to the O–H stretching vibration and a small amount of absorbed H2O.30,31 Furthermore, it was found that the shape of the FTIR spectra in all ACN samples remained almost unchanged.
Fig. 2 presents the FESEM images of the ACN nanocomposite samples. The as-prepared g-C3N4 sample exhibits a morphology of overlapping layered sheets, resembling a graphite-like structure. When silver nanoparticles decorate the g-C3N4 surface, a noticeable change in surface morphology is observed. As the amount of AgNPs in the nanocomposite sample increased, a progressive accumulation of Ag NPs on the g-C3N4 surface was evident, forming clusters of particles (samples ACN03, ACN07, ACN10 and ACN20).
![]() | ||
Fig. 2 FESEM images of the ACN nanocomposite samples: (a) g-C3N4, (b) ACN03, (c) ACN07, (d) ACN10, and (e) ACN20. (f) EDX spectrum of the ACN07 sample. |
To determine the silver content in the sample and compare it with theoretical calculations, the atomic compositions of the g-C3N4 and ACN07 samples were analyzed by energy dispersive X-ray spectroscopy (EDX). Fig. 2f shows the EDX spectrum results of the ACN07 sample. In the EDX spectrum, the characteristic peaks of the elements C, N and Ag appear, proving that in sample ACN07, there are elements C, N and Ag. Hence, the ACN nanocomposites possess high purity.
To further analyze the surface morphology of the composites, transmission electron microscopy (TEM) images of the CN and ACN07 samples were obtained and are shown in Fig. 3. The CN sample exhibits an uneven, layered structure with an irregular morphology. In contrast, the ACN07 sample shows the presence of small, dispersed particles which are attributed to the incorporation of Ag NPs into the g-C3N4 matrix.
Fig. 4a shows the reflectance spectra of the ACN nanocomposite samples. It is observed that the reflectance of the ACN nanocomposite samples remarkably increases when incorporating Ag nanoparticles. Moreover, the reflectance edge also shifts to a longer wavelength when the content of Ag increases, which implies more absorbance of visible light. The reason for this redshift is believed to be due to the plasmonic properties of silver nanoparticles in nanocomposite samples, which effectively absorb most of the light in the visible and infrared regions.
To further study the optical properties of the nanocomposite samples and evaluate their efficiency in visible-light-induced applications such as photocatalysis under solar irradiation, the optical bandgaps of the nanocomposite samples were extracted from the derivative method based on the Kubelka–Munk equation32,33 and expressed as
![]() | (1) |
The first derivative induced optical bandgaps of ACN nanocomposite are shown in Fig. 4b, and Fig. 4c shows that the optical band gap energy decreases with increasing silver content. This result might originate from the increase of absorbance due to the plasmonic resonance properties of Ag in the nanocomposites.
The PL fluorescence spectra of g-C3N4 and ACN07 samples, shown in Fig. 4d, indicated that the maximum emission of g-C3N4 (CN) is ∼435 nm and it has a higher intensity than the ACN07 sample, consistent with the results observed in the UV vis absorption spectra. This proves that the regeneration rate of photogenerated carriers in g-C3N4 is faster. In contrast, in the ACN07 sample, the recombination rate is slower or the lifetimes of electrons and holes are longer. This means that the photocatalytic ability is enhanced, because the longer the electrons and holes exist, the more carriers participate in the toxic compound decomposition reactions, leading to higher treatment efficiency.
The graphs of RhB concentration dependence on reaction time are shown in Fig. 5b. Over 30 minutes, during adsorption–desorption equilibrium in the dark, RhB concentration decreased by about 5–15%. After 75 minutes of illumination, the RhB was almost completely decomposed. The ACN07 sample gives the fastest decomposition of RhB solution, with an efficiency of 93.9%, followed by samples ACN00 and ACN03, which are slightly lower at 92.2% and 91.7%. The ACN10 and ACN20 samples showed relatively low efficiencies, with 81.67% and 77.52% (Fig. 5c), respectively. Thus, the photocatalytic efficiency of the Ag@g-C3N4 nanocomposite sample depends on the Ag ratio.
The photocatalytic reaction rate is expressed through the Langmuir–Hinshelwood kinetic equation
![]() | (2) |
![]() | (3) |
Fig. 5d shows the interpolated linear function according to the experimental data of each ACN nanocomposite sample and the R2 coefficient. Table 2 gives the kapp rate constants and R2 constants of the ACNx nanocomposite samples. The R2 coefficients of all nanocomposite samples are greater than 0.97, so the Langmuir–Hinshelwood model relatively appropriately reflects the photocatalytic process for RhB of the ACN nanocomposite samples. The ACN07 sample has the best photocatalytic ability (k = 0.039 min−1). It is possible that silver nanoparticles in nanocomposites act not only as an electron pool but also to capture the photoinduced electrons.
Sample | The content of Ag (wt%) | Activity (%) | k app (min−1) | R 2 | TONAg | TOFAg × 10−4 (min−1) |
---|---|---|---|---|---|---|
g-C3N4 | 0 | 53.92 | 0.009 | 0.986 | — | — |
ACN03 | 3 | 91.80 | 0.033 | 0.977 | 0.231 | 30.76 |
ACN07 | 7 | 93.92 | 0.039 | 0.970 | 0.101 | 13.49 |
ACN10 | 10 | 81.67 | 0.027 | 0.976 | 0.062 | 8.21 |
ACN20 | 20 | 77.52 | 0.019 | 0.980 | 0.029 | 3.90 |
In the catalytic system, TON and TOF are two important parameters used to evaluate the lifetime and performance of a catalyst.39 Therefore, TOF per unit amount of Ag NPs (Table 2) was used to evaluate the effect of Ag doping on the material properties. The ACN07 sample has the highest TOF of 30.76 min−1. When the Ag doping amount increases, the TOF decreases. This phenomenon occurs because when Ag increases, the amount of metal on the surface increases but its dispersion on the surface decreases. However, the opposite TON and TOF values also indicate that ACN has higher photocatalytic activity than pure g-C3N4. Therefore, there was a beneficial interaction between Ag and the g-C3N4 matrix. For details of the TON and TOF calculations, please see the ESI.†
The catalyst dosage also affects the dye decomposition efficiency. If the catalyst dosage is low, it is not enough to create active centers for the dye adsorption process on the catalyst surface, so the dye decomposition efficiency will decrease. If the catalyst dosage is too high, it will block the incident light and reduce light absorption, leading to a decrease in the ability to trap light and preventing the generation of photogenerated electrons and holes, so the dye decomposition efficiency will also decrease. Therefore, an optimal balance between RhB adsorption capacity and photon collection capacity will be achieved with the optimal catalyst dosage, and the efficiency will be optimized.
Fig. 6a presents the degradation of RhB using the ACN07 nanocomposite at different dosages (50–100 mg). The catalytic reaction rate was significantly enhanced with the dosage of catalyst. To evaluate the effect of dosage on the catalytic performance, the ratio of reaction rate to dosage was calculated. The performance ranking was as follows: 70 mg > 60 mg > 50 mg > 80 mg > 100 mg. Thus, the best sample dosage was 70 mg. Similarly, the RhB degradation reaction rate was affected by the concentration of RhB used (Fig. 6b). At low RhB concentration (5 ppm), the degradation rate of RhB increased significantly compared to that at high concentration (30 ppm), because when the RhB concentration is too high, the adsorption of RhB onto the catalyst decreases. The optimal RhB concentration in this study was 10 ppm.
![]() | ||
Fig. 6 Effects of (a) the dosage of ACN07 and (b) concentration of RhB solution on photocatalytic activity. |
The photocatalytic performance of RhB decolourization largely depends on the generation of strong chemically active radicals during the reaction process. The primary active species typically considered include hydroxyl radicals (˙OH), superoxide radicals (˙O2−), and photogenerated holes (h+). In this work, to study the effects of chemically active radicals, three agents were used: benzoquinone (BQ), isopropanol (IPA), and sodium oxalate (NO) for the radicals superoxide (*O2−), hydroxyl (*OH−) and hole (h+), respectively. In each experiment, 1 ml of the agent with a 1 mM concentration of the respective scavenger was added into a beaker containing 50 ml of 10 ppm RhB solution containing 0.07 g ACN07. The corresponding decolourization efficiencies in the presence of the agents are shown in Fig. 7a.
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Fig. 7 (a) Effect of scavengers. (b) Cycling runs, (c) XRD patterns and (d) FT-IR spectra of the ACN07 sample initially and after the fourth cycle. |
The role of reactive species in the photocatalytic degradation of RhB was further investigated through radical scavenging experiments. The addition of isopropanol has little effect on the reaction rate. Thus, it can be confirmed that the hydroxyl radical (*OH−) is not essential in the decomposition process of RhB dye. Interestingly, in the presence of the NO scavenger, the photocatalytic activity of the Ag@g-C3N4 nanocomposite sample increases, so h+ is not the active substance in this photodegradation process. In the presence of BQ, the reaction rate decreased the most. At the same time, it was observed that the peak shift phenomenon occurred relatively little, but the spectrum gradually increased with illumination time. The spectral enhancement becomes stronger when moving towards short wavelengths. The photodegradation of the RhB dye was significantly inhibited in the presence of BQ, demonstrating that O2− plays a major role in this process.
These results demonstrate that h+ and especially O2− are the main reactants in the photocatalytic RhB decomposition. The reusability of the Ag@g-C3N4 photocatalyst was evaluated by four consecutive photocatalytic runs, as seen in Fig. 7b. For each recycling, the photocatalytic material was filtered using a vacuum system to collect the residue. The resulting residue was dried in a dryer at 80 °C for 24 h. Then, the material was ground and photocatalyzed under similar conditions (material weight 0.07 g, RhB dye volume 50 ml at 10 ppm concentration).
RhB photodegradation efficiency was almost complete in each cycle. Therefore, there was no significant loss of catalytic activity even after 4 cycles. Therefore, the Ag@g-C3N4 nanocomposite is reusable.
Fig. 7c and d show the XRD and FTIR results of the ACN07 sample initially and after the cycling. It is easy to see that the diffraction peaks of the ACN07 sample hardly change after 4 cycles (Fig. 7c). This means that the ACN07 sample has good repeatability and stability. The FTIR measurement results of this sample are consistent with the XRD measurement results.
The photocatalytic enhancement mechanism of RhB degradation by ACN nanocomposite can be described as shown in Fig. 8. The EVB and ECB values of the Ag@g-C3N4 nanocomposites can be calculated by the equations40
![]() | (4) |
![]() | ||
Fig. 8 Proposed mechanism for the improved photocatalytic behaviour toward RhB over the ACN composite under LED illumination. |
The values of ECB and EVB for g-C3N4 are estimated to be −1.24 eV and 1.70 eV, respectively.
The reaction process is described in eqn (5)–(8) and is detailed as follows. Under the irradiation of visible light, only g-C3N4 absorbs visible light and is excited. Then, the electrons in the VB can be transferred to the CB of g-C3N4 to generate photogenerated electron pairs. Due to the SPR effect of silver in the form of nanoparticles, the generation rate of e–h pairs of g-C3N4 increases.41,42 Finally, the ˙O2− species photodegraded RhB into H2O and CO2 as follows.
g-C3N4 + hν → g-C3N4(e− + h+) | (5) |
g-C3N4(e−) → AgNPs(e−) | (6) |
AgNPs@g-C3N4(e−) + O2 → *O2− | (7) |
*O2− + RhB → CO2 + H2O | (8) |
Table 3 summarizes the RhB degradation performance of the ACN07 sample compared with some published results. ACN07 has a very good RhB degradation efficiency of up to 95% in 75 min. Moreover, the reaction can be carried out with an LED lamp (150 W, λ ≥ 450 nm). The sample has high stability after 4 cycles. The results indicate the applicability of ACN samples in wastewater treatment.
Photocatalyst | Light source | Dosage (mg) | Dye concentration (ppm) | Volume of dye (ml) | Reaction time (min) | Removal efficiency (%) | Ref. |
---|---|---|---|---|---|---|---|
Ag-(P/CNNS) | Xe lamp 300 W | 25 | 10 | 50 | 240 | 98 | 43 |
a-AgSiO/CNNS-500 | Xe lamp 500 W | 50 | 10 | 50 | 150 | 95 | 44 |
Ag@g-C3N4 NSs | Xe lamp 400 W | 2 | 10 | 20 | 250 | 89 | 45 |
0.02Ag/g-C3N4 | 100 W | 20 | 5 | 100 | 25 | 97 | 46 |
AgI/g-C3N4 | Osram, 125 W | 50 | 5 | 50 | 120 | 80 | 47 |
ACN07 | LED lamp, 150 W | 70 | 10 | 50 | 75 | 95 | This work |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d5na00552c |
This journal is © The Royal Society of Chemistry 2025 |