Open Access Article
Adriana
Popa
a,
Maria
Stefan
a,
Sergiu
Macavei
a,
Lucian
Barbu-Tudoran
ab,
Ioana
Perhaita
c,
Maria
Suciu
a,
Cristian
Leostean
a and
Dana
Toloman
*a
aNational Institute for Research and Development of Isotopic and Molecular Technologies, Donat 67-103, Cluj-Napoca, 400293, Romania. E-mail: dana.toloman@itim-cj.ro
bElectron Microscopy Center, Faculty of Biology and Geology, Babes-Bolyai University, Clinicilor 5-7, 400006, Cluj-Napoca, Romania
cBabes-Bolyai University, Raluca Ripan Institute for Research in Chemistry, Fantanele 30, Cluj-Napoca, 400294, Romania
First published on 3rd February 2026
In the present research, ZnO:Mn rods obtained from recycled anodic paste of spent Zn–MnO2 alkaline batteries were immobilized on the surface of graphitic carbon nitride (gC3N4) and tested as photocatalysts for degradation of RhB under visible light irradiation. The effect of the ratio between the two components of the composite materials on the RhB removal rate was investigated. The achievement of the composite material was proved by X-ray diffraction (XRD), scanning transmission electron microscopy (STEM), Fourier transform infrared spectroscopy (FTIR), and electron paramagnetic resonance (EPR). The Brunauer–Emmett–Teller (BET) analysis shows that increasing the ZnO:Mn content decreases the surface area of the composite samples. The composite samples show enhanced photocatalytic activity under visible irradiation compared with ZnO:Mn. The sample with the ratio 1–0.1 between gC3N4 and ZnO:Mn has the highest removal rate of 93% with a kinetic constant of 12.1 × 10−3 min−1 almost six times higher than that corresponding to the ZnO:Mn sample (2.3 × 10−3 min−1). The superoxide radicals are the main reactive oxygen species (ROS) involved in the dye degradation, as evidence by EPR spectroscopy coupled with the spin trapping technique. The coupling between gC3N4 and ZnO:Mn suppresses the electron–hole pair recombination, improving the photocatalytic performance. Moreover, the sample has good stability, and the removal rate was slightly modified after 5 consecutive reaction cycles. Also, the samples have a potential inhibitory antibacterial effect.
Many techniques were developed to treat contaminated water, such as filtration, coagulation, flocculation, adsorption, and physical and chemical methods. Unfortunately, all these methods have limitations in removing organic pollutants and heavy metals.4 One of the promising technologies for mitigating environmental pollution is photocatalysis, an advanced oxidation process. Photocatalysis has good efficiency in degrading organic contaminants and heavy metal ions. The photocatalytic process is explained by the activation of the semiconductor material by light irradiation with energy equal to or higher than its band gap energy. Thus, electron–hole pairs are generated, which can participate in organic pollutants' oxidation and reduction reactions. Researchers have recently focused on developing photocatalytic materials,5–7 improving existing catalysts via synthesis methods or elaborating new ones.
ZnO, an n-type metal oxide semiconductor, is a common photocatalyst with high oxidation capacity, adjustable size, excellent chemical stability, low toxicity and can be synthesized by different methods. ZnO shows a higher absorption capacity covering a large fraction of the solar spectrum than TiO2.8 One of its limitations is a relatively high charge carrier recombination, negatively impacting the photocatalytic reactions. To overcome this limitation, various methods have been applied. Doping with nonmetal and metal ions successfully narrows the band gap, enhances the separation charge carrier, and shifts the wavelength of absorbed light to the visible area.9,10
The coupling of ZnO with a narrow energy band gap semiconductor represents another method of enhancing the photocatalytic activity. In this case, a heterostructure is obtained at the interface of the two semiconductors. The photogenerated electrons would move from the semiconductor with a higher conduction band energy to the lower one, enhancing the separation of photogenerated electrons and holes.11 The coupling between ZnO and g-C3N4 was reported as an encouraging solution due to the band structure matching, leading to the accumulation of spatial charges at the interface, facilitating the separation of photogenerated charges. Besides, the obtained composite can be activated by a broad light spectrum, particularly visible light.12 g-C3N4 is a non-metallic semiconductor with high thermal and chemical stability due to the strong covalent bonds between carbon and nitrogen atoms. With a narrow band gap (2.7 eV), g-C3N4 can absorb visible light and act as a responsive photocatalyst. Its limits are related to the high recombination process, weak electrical conductivity, and low oxidation ability of holes in the valence band.13
Recently, different composite materials based on ZnO and g-C3N4 have been reported with enhanced photocatalytic performances under visible light. Hassan et al. developed ZnO/g-C3N4 S-scheme photocatalysts used for paracetamol degradation, and proved that hydroxyl radicals are the reactive species involved in paracetamol photodegradation.14 X. Gao et al. obtained g-C3N4 nanosheets decorated with ZnO nanoparticles by refluxing method at low temperature and obtained composites with enhanced photocatalytic activity.15 Also, K. Bi et al. reported ZnO/g-C3N4 S-scheme with effective separation of photogenerated charges and improved photocatalytic material for RhB degradation.16 These reports indicate that ZnO/g-C3N4 composite material has promising potential in wastewater treatment by optimizing the band structure at the composite interface.
In the last years, the waste-derived nanomaterials have represented one of the emerging research areas. Numerous efforts have been made for the nanomaterial's synthesis from diverse biological and industrial wastes. Around 7 billion tons of industrial waste are generated or disposed of annually, which negatively impacts the environment due to their toxic, flammable, corrosive, highly reactive, infectious, and radioactive properties.17 Consequently, it is important to recycle these industrial wastes to obtain added-value products that benefit environmental safety. About 90% of the total annual transactions of portable batteries worldwide are represented by Zn–Mn batteries. Therefore, recycling Zn from Zn–Mn battery waste fosters the sustainable use of resources and prevents the disposal of these contaminants into the environment. The Zn–Mn battery waste recycling has been used to obtain nanomaterials such as ZnO nanoparticles,18 nanofibers,19etc.
Considering the above, this work focuses on preparing gC3N4-ZnO:Mn composites with enhanced photocatalytic activity for water depollution under visible irradiation. Mn-doped ZnO particles were obtained from anodic paste of spent Zn–MnO2 alkaline batteries.20 The decoration of Mn-doped ZnO particles on the gC3N4 surface was realized using poly(allylamine) hydrochloride (PAH) as a linking agent. Various characterization methods characterized the composite samples, and their photocatalytic activity was evaluated using a synthetic RhB solution as a model pollutant. The photocatalytic mechanism was explained based on the EPR spin trapping method results and in correlation with the other characterization techniques. The heterojunction photocatalysts based on Mn-doped ZnO particles and gC3N4 exhibit enhanced photocatalytic properties due to the photogenerated charges, which are better separated.
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ROS generation was evidenced by EPR spectroscopy coupled with the spin trapping method. As spin trapping reagent was used DMPO. 10 mg of composite sample was dispersed in DMSO (1 mL) and homogenized in an ultrasound bath (30 min) before use. DMPO of 0.2 mol L−1 concentration was added to the above mixture. The fresh prepared samples were immediately transferred into the quartz flat cell optimized for liquids measurements. All tests were performed in the same conditions.
To evidence the active species involved in the photocatalytic degradation process of RhB under visible irradiation, the scavenger experiments were performed. The following scavengers were used vitamin C for superoxide radical, and isopropyl alcohol for hydroxyl radical. In this experiment was added scavenger agents to the initial solution keeping the photodegradation experiments described above identical.
The stability of the sample was analyzed using reutilization tests. Before each run, the catalyst was recovered by centrifugation and then thoroughly washed with water and ethylic alcohol and dried overnight.
Bacterial cytotoxicity. Escherichia coli (ATCC 25922) and Staphylococcus aureus (ATCC 12598) colonies were collected from Muller-Hinton-Agar media and resuspended in 0.9% saline solution to a density of 0.5 McF. From this inoculum, new MH-Agar plates were seeded using sterile cotton swabs and then sterile cotton disks were applied on top for the disk diffusion method. The 10 mg mL−1 gC3N4-ZnO:Mn_1–0.1 disks were placed on the agar medium and the cotton disks were impregnated with 100 µL of 10 mg mL−1 RhB and with 10 mg mL−1 gC3N4-ZnO:Mn_1–0.1 resulting solution. Antibiotics pre-loaded disks were used as controls: kanamycin 30 µg mL−1, gentamycin 10 µg mL−1, ciprofloxacin 5 µg mL−1. Plates were placed in the incubator in dark conditions at 37 °C for 24 hours, after which the developed hallows were measured and the plates were photographed.
To investigate the structure of the composite materials, XRD characterization was performed. The obtained XRD patterns corresponding to gC3N4-ZnO:Mn composites samples are shown in Fig. 2a in comparison with the specific patterns of gC3N4 and ZnO:Mn. The XRD patterns of all prepared composite materials reveal the presence of ZnO specific peaks indexed with the wurtzite hexagonal structure (PDF 01-070-8072). In addition to these, the diffractograms contain a pronounced peak at 27.4° characteristic of graphitic systems (PDF 00-050-1249). The peak located at 27° was assigned to the interplanar stacking peak of the aromatic systems indexed to the (002) peak.22,23 No characteristic peaks of secondary phases of other impurities were observed. For ZnO, the mean crystallite size is about 140 nm; the evaluation was made by the Williamson–Hall (W–H) method.
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| Fig. 2 Diffraction patterns of gC3N4-ZnO:Mn composites sample (a); FT-IR spectra of gC3N4 and gC3N4-ZnO:Mn_1–2 composite sample (b). | ||
FT-IR spectroscopy was performed to obtain more structural information about the functional groups on the sample's surface. In Fig. 2b are illustrated the spectra corresponding to gC3N4-ZnO:Mn_1–2 compared with the spectrum of gC3N4. The gC3N4 spectrum analysis indicates the presence of an intense band located at 1637 cm−1,24 due to C
N stretching and several bands in the range of 1544 cm−1 and 1235 cm−1 attributed to the vibration modes of the C–N bonds from the CN aromatic unit.24 It can also be observed the existence of a band located at 807 cm−1 specific to the triazine units from gC3N4.25 The composite clearly displays all of the FTIR vibration peaks associated with gC3N4, which shows that the structure of gC3N4 remains unmodified during the decoration process. Moreover, the composite samples contain a supplementary band located in the range 400–600 cm−1, which is specific to the vibration of the Zn–O bond.26
The EPR spectroscopy was used to prove the paramagnetic species in the composite samples; the obtained spectra for all the samples are displayed in Fig. 3a. To get deep insight into the paramagnetic species responsible for the obtained resonance signals, a simulation of the spectrum corresponding to gC3N4-ZnO:Mn_1–2 sample was performed (Fig. 3b). From the simulation analysis results that resonance signals are due to the overlapping of three resonance signals. Signal S1, consisting of a well-resolved hyperfine structure characteristic of isolated Mn2+ ions, originated from the interaction between the S = 5/2 electronic spin and the I = 5/2 nuclear spin of the 55Mn nucleus. The following Hamiltonian parameters: g-tensor, g = 2.0018, hyperfine coupling constant, A = 222 MHz, and zero-field parameter, D = 702 MHz were used for simulation. Signal S2, a sharp one, with a linewidth of 6 G situated at g ∼ 2.006, is attributed to the generation of unpaired electrons in the localized π-conjugated structure of gC3N4.27,28 The broad resonance line signal S3 is probably due to some agglomerated Mn2+ ions.29 The presence of Mn2+ ions is due to the inter-contamination between the anode and cathode from the spent batteries.20
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| Fig. 3 Experimental EPR spectra of gC3N4-ZnO:Mn samples (a); experimental and simulated EPR spectra of gC3N4-ZnO:Mn_1–2 sample (b). | ||
Morphological characteristics were investigated by SEM and TEM microscopy. Fig. 4a and b are illustrated, as examples of SEM and TEM images for the gC3N4-ZnO:Mn_1–1 sample. The SEM and TEM images indicate the presence of both gC3N4 layers and ZnO particles. The ZnO particles have a rod shape with the length varying between 500 nm and 1.5 µm and a thickness of 200 nm. Similar morphology and particle size were observed for all samples. To confirm the presence of both components, the elemental mapping was performed by EDS (Fig. 4c). The following elements were evidenced: N and C atoms from gC3N4 layers and Zn, O atoms from ZnO particles.
The specific surface area and porosity measurements were carried out because porosity can significantly impact the specific properties of materials. The porosity of the samples was measured according to Barrett, Joyner, and Halenda (BJH) method and adsorption/desorption procedures. The porosity analysis reveals varied characteristics of composite samples concerning the synthesis conditions, as illustrated in Fig. 5(a–d).
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| Fig. 5 N2 adsorption/desorption isotherm and pore size distribution (BJH) of gC3N4 (a), gC3N4-ZnO:Mn_1–0.1 (b), gC3N4-ZnO:Mn_1–1 (c), and gC3N4-ZnO:Mn_1–2 samples (d). | ||
The investigated samples exhibit similar isotherms of type III, which are typical of low-porous adsorbents, and the hysteresis created by the two adsorption–desorption isotherms is of type H3. This type of hysteresis appears in aggregates of flat particles or adsorbents with crack-like pores. The pore volume distribution curves as a function of diameter exhibit a multimodal shape, indicating the presence of dimensionally irregular pores. As the gC3N4-ZnO:Mn ratio increases, the pore volume increases from 0.115 cm3 g−1 (gC3N4) to 0.261 cm3 g−1 (gC3N4-ZnO:Mn_1–1), then drops dramatically to 0.054 cm3 g−1 at a ratio of 1
:
2. The gC3N4 sample's maximum at 31 nm indicates a high level of mesopores (D < 50 nm). At a ratio gC3N4-ZnO
:
Mn of 1
:
0.1, the mesopores (32 nm) clog slightly and become shorter, but unlike the gC3N4 sample, macropores (275 nm) predominate, as seen by an increase in the average pore diameter from 31.15 nm (gC3N4) to 92.04 nm (1
:
0.1). At a 1
:
1 ratio of components, the pores get longer, with macropores (97 nm) dominating. When the ratio gC3N4-ZnO
:
Mn is 1
:
2, the pores clog, and the messo-macropore ratio equalizes. The specific surface area of the composite samples decreases by increasing the content of ZnO:Mn from 13.64 m2 g−1 in case of gC3N4 to 4.78 m2 g−1 for gC3N4-ZnO:Mn_1–2 due to the gC3N4 pore blocking by the addition of ZnO:Mn. Table 1 illustrates the main characteristics, including the surface areas (SBET), pores volume, and pores diameter of all the samples.
| Sample | S BET (m2 g−1) | Pores volume (cm3 g−1) | Pores diameter (nm) |
|---|---|---|---|
| g-C3N4 | 13.64 | 0.115 | 31.15 |
| gC3N4-ZnO:Mn_1–0.1 | 11.38 | 0.218 | 92.04 |
| gC3N4-ZnO:Mn_1–1 | 12.57 | 0.261 | 24.76 |
| gC3N4-ZnO:Mn_1–2 | 4.78 | 0.054 | 41.44 |
| ZnO:Mn | 2.60 | 0.018 | 33.6 |
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| Fig. 6 UV-vis spectra (a); Tauc's plots (b); PL spectra (c) of gC3N4 and gC3N4-ZnO:Mn samples; and PL spectra of the gC3N4 sample together with deconvoluted peaks (d). | ||
Photoluminescence analysis was used to assess the samples' e-h separation efficacy. Photoluminescence emissions on semiconductors result from the radiative recombination of photoelectrons and produced holes.31Fig. 6c shows the PL spectra of the gC3N4-ZnO:Mn composite samples compared with that of gC3N4 obtained using an excitation wavelength of 325 nm. The PL spectra are similar for all the samples and consist of a broad emission band covering the blue-violet to green light region. The experimental spectra were deconvoluted using a Gaussian fitting function to highlight the emission bands and their assignment better. Fig. 6d shows, as an example, the spectrum of gC3N4 obtained after deconvolution. The deconvolution of the gC3N4 sample reveals the presence of three bands located at 454 nm, 489 nm, and 543 nm. According to previous PL studies, the luminescence properties of gC3N4 are due to the energy states of sp3 hybridized C–N σ band, sp2 C–N π band, and the lone pair (LP) of the bridging nitrogen atom. Thus, the PL emission band centered at 454 nm was attributed to the σ*–LP transition, while the emission band at 489 nm was related to the transition of the electrons relaxed at π* and LP state, and that at 543 nm to π*–π band transition.32,33 By decorating gC3N4 with ZnO:Mn, the emission is quenched, meaning that the recombination process is delayed, so the photogenerated charges are better separated, beneficial for the photocatalytic process.
The composite samples show enhanced photocatalytic activity under visible irradiation compared with ZnO:Mn. The sample with the lower content of gC3N4 has the highest removal rate of 93%. To describe the photocatalytic process first-order kinetic model was applied, and the obtained plots are illustrated in Fig. 7b; the obtained kinetic constants are inserted in the inset. Indeed, gC3N4-ZnO:Mn_1–0.1 has the best removal rate, with the kinetic constant being almost six times higher than that corresponding to the ZnO:Mn sample.
To evaluate the photocatalytic mechanism, the reactive oxygen species generated by the samples were evidenced by EPR spectroscopy coupled with the spin trapping method. The sample with the best photocatalytic activity was chosen to evidence the ROS generation, and as a spin trapping agent, DMPO was used. Before irradiation, no spectrum was obtained, but after 25 min of visible light irradiation, as observed in Fig. 8a, a spectrum composed of several components was obtained. To extract the components' spectrum, a simulation was performed.
The linear combination of the following spin adducts was obtained: ˙DMPO-O2− (aN = 12.8 G, aβH = 10.4 G, aγH = 1.39 G, g ∼2.009) and ˙DMPO-N2 (aN 14 G, g ∼2.009). Superoxide radicals ˙O2− results from the interaction between the photogenerated electrons and adsorbed O2. The second component is ˙DMPO-N, which appears by the N–C bond cleavage of DMPO.34 This result indicates that the sample generates superoxide radicals ˙O2− under visible irradiation, which means that the CB position is more negative than the potential of O2/˙O2−, it doesn't generate hydroxyl radicals, probably because the VB position is less positive than the potentials of H2O/˙OH and OH−/˙OH.28
The scavenger experiments were conducted to identify the reactive oxygen species involved in the photodegradation of RhB. Vitamin C was used as a scavenger for ˙O2−, while isopropanol targeted ˙OH. To check influence of the scavenger concentration on the photocatalytic activity of the gC3N4-ZnO:Mn_1–0.1 sample, the concentration of the scavenger agents was varied between 3 to 7 mM for vitamin C and 60 to 140 µL/10 mL RhB solution for isopropanol. The obtained results are shown in Fig. S1. As was expected an increased concentration of the scavenger agent results in higher inhibition of the photocatalytic activity. As an example, Fig. 8b shows the photocatalytic activity of gC3N4-ZnO:Mn_1–01 sample in the absence and presence of 5 mM vitamin C and 100 µL isopropanol added to the initial RhB solution. The addition of both scavengers induced a decrease in the photodegradation rate. Notably, vitamin C caused the most significant inhibition of RhB degradation, indicating that while both reactive species contribute to the process, ˙O2− plays the dominant role.
Consequently, the proposed photocatalytic mechanism is the following: when visible light irradiates the composite sample, the electrons from the valence band (VB) of gC3N4 are excited to its conduction band (CB). Because the g-C3N4 LUMO edge potential is more negative compared with that of ZnO, the photoinduced electrons from the LUMO of g-C3N4 will be transferred easily to that of ZnO via the interface,35 and here they will react with the O2 molecules adsorbed on the photocatalyst surface, generating superoxide radicals able to degrade the pollutant molecules. At the same time, the holes from the VB of ZnO migrate to the HOMO of g-C3N4, but since its position is lower than the oxidation potential of H2O/˙OH and OH−/˙OH redox pair, these reactions may not take place. Thus, only the remaining holes in the ZnO VB could participate in oxidation reactions. The proposed scheme of the photocatalytic mechanism obtained based on the valence band position evaluated by XPS (Fig. S2) and energy band gap values, and ROS generated by the sample is illustrated in Fig. 8c.
Furthermore, the reusability of the sample possessing the best photocatalytic activity (gC3N4-ZnO:Mn_1–0.1) was evaluated and illustrated in Fig. 8d. Only a slight decline in photocatalytic activity is observed after five consecutive reaction cycles measured under the same conditions, indicating that the prepared composites maintain good stability. The chemical stability of the photocatalyst was analyzed using XRD and FT-IR. Fig. S3 and S4 illustrate the XRD diffractogram and FT-IR spectra of the gC3N4-ZnO:Mn_1–0.1 sample before and after reusability tests showing no modification of the sample crystalline structure, sustaining its excellent chemical stability.
To highlight the potential application of the sample as visible light photocatalyst, the photocatalytic performance of the gC3N4-ZnO:Mn_1–0.1 sample was compared with reported studies. Table 2 shows the comparison of the photocatalytic activity of various g-C3N4/ZnO based photocatalyst. The results show that gC3N4-ZnO:Mn_1–0.1 sample photocatalytic performance is comparable to those obtained in the literature with the specification that the current state of the tests was done on RhB, and the results in the literature were obtained using other types of pollutants.
| Catalyst | Light source | Pollutant | Irradiation time (min) | Degradation (%) | Kinetic ct. (min−1) | Ref. |
|---|---|---|---|---|---|---|
| g-C3N4/ZnO | Visible | MB | 60 | 76 | 0.023 | 36 |
| g-C3N4/ZnO:Ni | Solar | MB | 70 | 100 | 0.031 | 37 |
| g-C3N4/ZnO | Solar | Paracetamol | 60 | 95 | 0.052 | 38 |
| g-C3N4/ZnO | Visible | MB | 240 | — | 0.007 | 39 |
| g-C3N4/ZnO:Mn | Solar | MB | 60 | 98 | 0.032 | 40 |
| g-C3N4/ZnO:Mn | Visible | RhB | 180 | 93 | 0.012 | Present work |
The supplementary information contains: the influence of different concentrations of scavengers on the removal rate; XPS spectra; XRD diffractogram and FT-IR spectra of the sample before and after reusability tests. See DOI: https://doi.org/10.1039/d5ma01238d.
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gC3N4 incorporation on the photocatalytic dye decomposition of ZnO film coated on stainless steel wire meshes, J. Mater. Sci: Mater. Electron., 2019, 30, 19703–19717, DOI:10.1007/s10854-019-02321-w.| This journal is © The Royal Society of Chemistry 2026 |