3.1. Structural Characterization
The PXRD analysis of the CQDs/FeO
x composite (CQDs/FeO
x–3 sample), FeO
x powder (achieved through the calcination of IOS at 300 °C), and IOS (raw material) is depicted in
Figure 2. Evidently, the waste IOS contained two main phases. Among them, the characteristic peaks at 30.0°, 35.4°, 37.0°, 43.1°, 56.9°, and 62.5° corresponded to the (220), (311), (222), (400), (511), and (440) crystal planes, respectively, which could be attributed to magnetite (Fe
3O
4, JCPDS card no. 19-0629). Additionally, the characteristic peaks at 33.1° and 35.6° could be attributed to the (104) and (110) crystal planes of hematite (α-Fe
2O
3, JCPDS card no. 33-0664). This indicated that the IOS mainly contained Fe
3O
4 and α-Fe
2O
3, with Fe
3O
4 being dominant. Combining this with the results of the elemental composition analysis (See
Table 2), the Fe/O mass ratio in the IOS was 2.59, and it could be calculated that there was only about 10.8% of α-Fe
2O
3 in the mixed phase of iron oxide. Typically, the band gap of magnetite (Fe
3O
4) was too small to exhibit an effective photocatalytic ability. As a result, the iron oxide photocatalytic component was mainly α-Fe
2O
3. Therefore, it was foreseeable that the waste IOS could not be directly used as a photocatalytic material or directly combined with CQDs due to the low content of α-Fe
2O
3, making calcination treatment necessary to enhance its photocatalytic potential.
Comparing the PXRD pattern of the FeOx powders obtained through the calcination of IOS at 300 ℃ with that of IOS, it was evident that the diffraction peaks of the α-Fe2O3 were significantly enhanced after calcination. The characteristic peaks at 24.1°, 33.1°, 35.6°, 40.9°, 49.5°, and 54.1° corresponded to the (012), (104), (110), (113), (024), and (116) crystal planes of α-Fe2O3, respectively. Additionally, based on compositional analysis, the Fe/O mass ratio decreased to 2.51, indicating that the FeOx powder contained 43.3% of α-Fe2O3. This transformation implied that calcination in air could convert a portion of the initially non-photocatalytic Fe3O4 into photocatalytically active α-Fe2O3, which laid the foundation for obtaining practical photocatalytic materials after the composite with CQDs. The PXRD patterns of the CQDs/FeOx composite and FeOx exhibited resemblances; however, the diffraction peaks corresponding to the CQDs within the composite were not prominently discernible due to their relatively modest concentration.
The results of the particle size distribution testing indicated that the obtained CQDs/FeO
x composite (CQDs/FeO
x–3 sample) exhibited a Z-average particle size value of 127.8 ± 63.26 nm (refer to
Figure S1 in ESI). The outcomes of the TEM analysis for the CQDs/FeO
x composite (CQDs/FeO
x–3 sample) are visually depicted in
Figure 3a. It could be observed that the CQDs/FeO
x composites exhibited an irregular lamellar structure, with uniformly dispersed spherical CQDs particles on the FeO
x surface. In
Figure 3b, the HRTEM image vividly revealed the intricate lattice arrangement of the FeO
x and CQDs. The lattice stripes, exhibiting spacings of 0.185 nm, 0.198 nm, and 0.271 nm, corresponded, respectively, to the (104), (110), and (024) crystal planes of α-Fe
2O
3. Furthermore, discernible lattice stripes with spacings of 0.103 nm and 0.168 nm aligned with the (111) and (220) crystal planes of Fe
3O
4. These observations indicated that the obtained FeO
x was primarily a mixture of magnetite (Fe
3O
4) and hematite (α-Fe
2O
3), which aligned with the PXRD results. Moreover, crystalline planes with a lattice spacing of about 0.283 nm, corresponding to the (020) crystalline planes of CQDs [
50,
51], were also observed, confirming the successful combination of the WRN-based CQDs and FeO
x in the resulting composite.
The XPS spectra of both the CQDs/FeO
x composite and FeO
x powders are displayed in
Figure 4 and summarized in
Table 3.
Figure 4a highlights the elemental presence of Fe, O, and C within the CQDs/FeO
x composite. Notably,
Figure 4b and
Table 2 elucidate that the Fe 2p spectra disclosed characteristic peaks at 724.67 and 710.49 eV, corresponding to the Fe(2p
1/2) and Fe(2p
3/2) signals, respectively. A noteworthy separation of divalent and trivalent iron signals was discernible within the Fe(2p
3/2) signal, indicative of the presence of both Fe
2+ and Fe
3+ ions in the resulting CQDs/FeO
x composite. In the high-resolution spectrum of O 1s, the CQDs/FeO
x complex displayed distinct Fe–O and C–O bonds, hosting characteristic signals positioned at 530.71 and 528.29 eV, respectively. In contrast, the O 1s spectrum of the FeO
x calcined at 300 °C displayed two distinct peaks at 530.5 and 529.38 eV, attributing them to the Fe–O bond and the hydroxyl group present on the FeO
x surface, respectively. This led to the inference that the interaction between CQDs and FeO
x involved the carboxyl group within the CQDs and the Fe–OH group on the surface of the FeO
x, leading to the vanishing of the surface hydroxyl signal and the emergence of the C–O bond signal, as indicated in
Figure 4c and
Table 3. Additionally, in the high-resolution C 1s spectrum of the CQDs/FeO
x composite, the peak at 283.69 eV could be attributed to the C–C bond within the CQDs. Simultaneously, the signals centered at 285.03 and 287.51 eV corresponded to the C–O and C=C bonds of CQDs, respectively, confirming the successful integration of the CQDs and FeO
x within the resultant composites.
As shown in
Figure 5a, without the combination of CQDs, the IOS and FeO
x exhibited an obvious Fe–OH stretching vibration peak at around 880 cm
−1 in their IR spectra. However, this peak disappeared after the composite of FeO
x with CQDs. Paired with the XPS findings, it is conceivable that the intricate interplay between the CQDs and FeO
x constituted a response involving the carboxyl group within the CQDs and the hydroxyl group located on the FeO
x surface. Furthermore, characteristic absorption peaks of CQDs were observed in the IR spectra of the CQDs/FeO
x composites, including the stretching vibration (3422 cm
−1) and bending vibration (1620 cm
−1) of the O–H bond on the CQDs, and the stretching vibration (1063 cm
−1) of the C–O bond, etc. In addition, due to the presence of organic groups such as hydroxyl and carboxyl groups in the CQDs, the PZC value of the CQDs/FeO
x composites (8.46) was higher than that of the non-composite FeO
x powder (7.98) (See
Figure 5b). In addition, due to larger feedstock particles, the CQDs/FeO
x composite exhibited a relatively low specific surface area (2.28 m
2 g
−1) compared with the CQDs/TiO
2 [
44] and CQDs/ZnO [
45] photocatalytic composites in our previous report; however, it was still slightly higher than that of the non-composite FeO
x powder (1.57 m
2 g
−1) (See
Figure 5c).
3.2. Photocatalytic Performance of CQDs/FeOx Composites
The resulting CQDs/FeO
x composite exhibited excellent photocatalytic degradation efficiency towards various organic pollutants.
Figure 6a underscores the formidable challenge of degrading methylene blue, a prevalent and highly toxic pollutant in dyeing wastewater, using 405 nm visible purple light. In the absence of a catalyst, its degradation rate remained at a mere 2.3%, even after an extended duration of 8 h (480 min). Due to its non-photocatalytic Fe
3O
4 component, the IOS itself lacked the ability for photocatalytic degradation to methylene blue, as its degradation rate was only 4.9% after 480 min of light irradiation, which was almost indistinguishable from the degradation without the catalyst. However, after calcination at 300 °C, a portion of the Fe
3O
4 in the IOS was converted into α-Fe
2O
3, resulting in the FeO
x with a certain photocatalytic degradation ability. The degradation rate of the FeO
x towards methylene blue reached 41.8% after 480 min of light irradiation, with an apparent degradation rate constant of 1.03 × 10
−3 min
−1. However, complete degradation could not be achieved under these conditions. In contrast, the catalytic effect of the CQDs/FeO
x composite (CQDs/FeO
x–3 sample) on methylene blue significantly improved after incorporating the WRN-based CQDs into the FeO
x. The composite demonstrated a good photocatalytic degradation rate (up to 99.30% within 480 min) and a relatively high degradation rate constant (5.26 × 10
−3 min
−1), enabling the complete degradation of methylene blue (See
Figure S2 in ESI).
It was found that achieving a good photocatalytic performance for the CQDs/FeO
x composite required the appropriate calcination of the IOS in an air atmosphere to enhance the content of α-Fe
2O
3. The degradation rates of methylene blue for CQDs/FeO
x composite materials obtained at different calcination temperatures (samples CQDs/FeO
x–1 to CQDs/FeO
x–5) are shown in
Figure 6b,c. Combined with the results of the phase and elemental composition, it was observed that without proper high-temperature calcination to increase the content of α-Fe
2O
3, even with the incorporation of CQDs, the catalytic effect could hardly be improved. For instance, the CQDs/FeO
x–1 sample obtained by heating the IOS at 100 °C had a Fe/O mass ratio of 2.59 due to the relatively low calcination temperature. It was found that only about 10.9% of α-Fe
2O
3 was present in the mixed FeO
x phase, similar to the IOS as a raw material. Consequently, despite containing CQDs, the photocatalytic degradation of CQDs/FeO
x–1 remained poor. After 480 min of light exposure, its degradation rate to methylene blue was only 35.79%, and the degradation rate constant was merely 7.04 × 10
−4 min
−1, which is even worse than the FeO
x sample without CQDs but calcined at 300 °C. There are reports indicating that, when heated in air at an appropriate temperature (around 300 °C), Fe
3O
4 exhibits a tendency to transform into α-Fe
2O
3 [
52,
53,
54]. As shown in
Table 1, with enhancing the calcination temperature, the Fe/O mass ratio of the composite FeO
x material showed a trend of initially decreasing and then increasing, indicating that the content of α-Fe
2O
3 first increased and then decreased. Among them, the CQDs/FeO
x–3 sample prepared with IOS calcined at 300 °C had the smallest Fe/O mass ratio (2.51), which corresponded to the highest α-Fe
2O
3 content (44%). Therefore, it exhibited the best photocatalytic performance and achieved the complete degradation of methylene blue within 480 min, with a degradation rate constant of 5.26 × 10
−3 min
−1. Furthermore, the material demonstrated excellent recyclability, and its degradation rate remained above 98% even after ten cycles of photocatalysis (See
Figure 6d). However, when compared to commercially available nanoscale TiO
2 or ZnO, the photocatalytic degradation efficiency of the obtained CQDs/FeO
x photocatalytic material was relatively low (See
Figure 6e,f). Nevertheless, due to its complete reliance on waste materials as feedstock, the cost of the CQDs/FeO
x photocatalytic material is significantly lower. Additionally, it possesses strong magnetism, unlike commercial TiO
2 or ZnO, enabling convenient recovery. Therefore, it may present a more competitive option for large-scale water purification.
Additionally, the loading amount of CQDs also affects the photocatalytic degradation capability of the CQDs/FeO
x composite material. As shown in
Figure 6g,h, at lower carbon contents, the photocatalytic degradation efficiency of the CQDs/FeO
x composite material improved with the increasing carbon content. The CQDs/FeO
x composite material with a carbon content of approximately 11 wt% (CQDs/FeO
x–3 sample) exhibited the best photocatalytic performance, with a degradation rate constant of 5.26 × 10
−3 min
−1 for methylene blue. However, it was found that further increasing the loading amount of CQDs may have an adverse effect on the photocatalytic performance. For example, in the case of the CQDs/FeO
x–7 sample featuring a carbon content of 20.2 wt%, a comparatively reduced degradation rate constant of 3.73 × 10
−3 min
−1 was observed for methylene blue degradation. This phenomenon could be attributed to the potential shielding influence stemming from the presence of carbon-based constituents [
55].
The obtained CQDs/FeO
x composite material could also be utilized for controlling antibiotic residues, as shown in
Figure 7. Under 405 nm purple light, the CQDs/FeO
x composite (CQDs/FeO
x–3 sample) could degrade 98.21% of tetracycline within 320 min, with an apparent degradation rate constant of 3.73 × 10
−3 min
−1. In comparison, under the same conditions, the FeO
x powder without CQDs could only degrade 40.45% of tetracycline, with an apparent degradation rate constant of 1.29 × 10
−3 min
−1.
Compared with other CQDs/iron oxide composites using different iron and carbon sources (
Table 4), the CQDs/FeO
x composite reported in this paper demonstrated a comparably good photocatalytic performance. Moreover, due to the complete utilization of waste materials (IOS and WRN) as raw sources, the synthesis cost of this material was significantly reduced compared to other CQDs/iron oxide composites [
29,
30,
31,
32,
33,
34]. This complete conversion of waste to treasure makes it more environmentally friendly and exhibits outstanding sustainability, making it more suitable for large-scale, industrial applications in water purification projects. In comparison to our previous reports on CQDs/TiO
2 and CQDs/ZnO composites based on WRN, the CQDs/FeO
x composite exhibited a weaker photocatalytic performance (See
Table 5). However, due to the presence of magnetic Fe
3O
4 components, it offers the advantage of simplified recovery procedures while ensuring high recyclability. Additionally, as the oxide component is derived from waste IOS, it eliminates the need for commercial reagents, further reducing the costs and promoting environmental friendliness.
3.3. Magnetic Properties of CQDs/FeOx Composites
In addition to exhibiting efficient photocatalytic degradation to various organic pollutants, the resulting CQDs/FeO
x composite also demonstrated outstanding magnetic properties. The magnetization curves of the CQDs/FeO
x composite and the raw IOS were tested and are shown in
Figure 8a. The IOS powder exhibited remarkable soft ferromagnetism at room temperature, characterized by a low coercivity of 97.4 Oe, a low residual magnetization intensity of 5.2 emu/g, and a high saturation magnetization intensity of 5.8 emu/g, primarily attributed to the abundance of Fe
3O
4 particles in the material.
As mentioned earlier, after the process of calcination and compounding, the magnetic properties of the CQDs/FeOx composites slightly weakened due to the reduced Fe3O4 content. Nevertheless, its saturation magnetization intensity remained at approximately 54.6 emu/g, along with low coercivity (117.1 Oe) and residual magnetization intensity (5.8 emu/g). Therefore, the CQDs/FeOx composite still exhibits exceptional soft magnetic characteristics, making it a promising candidate for various magnetic applications.
As depicted in
Figure 8b,c, the magnetic properties of the CQDs/FeO
x composite material enable efficient and convenient recyclability in photocatalytic applications. Following the photocatalytic process, the CQDs/FeO
x composite can be effortlessly separated using a magnetic field, achieving a mass recovery rate of 99.62% after the initial photocatalytic cycle and 98.45% after ten cycles of photocatalysis. Additionally, iron oxide photocatalysts have demonstrated excellent environmental compatibility, with minimal toxicity to fish and algae [
56,
57,
58]. Consequently, the resulting CQDs/FeO
x photocatalyst holds significant promise for large-scale industrial water purification.
3.4. Photocatalytic Mechanism of CQDs/FeOx Composites
To delve deeper into the photocatalytic mechanism of the resulting CQDs/FeO
x composite, the UV-VIS diffuse reflectance spectra of both the FeO
x and the CQDs/FeO
x composite are illustrated in
Figure 9a. Evidently, even after calcination at 300 °C, the main energy absorption region of the FeO
x inorganic phase was in the ultraviolet region, with almost no absorption in the visible wavelength range above 380 nm. In contrast, the CQDs/FeO
x composite material exhibited strong absorption throughout the entire visible light region, indicating that the introduction of CQDs enabled the composite material to utilize the energy in the visible light region more effectively, thereby generating more electron-hole pairs. Moreover, the determination of band gaps for the FeO
x and CQDs/FeO
x samples was performed through the application of the Tauc plot method [
59,
60], as depicted in
Figure 9b. The band gap of the FeO
x was 2.17 eV, but after introducing CQDs, the band gap of the CQDs/FeO
x composite material was further reduced to 1.40 eV. This narrower band gap allowed for more the effective utilization of energy in the visible light region, significantly promoting electron transitions and enhancing the photocatalytic degradation performance.
The valence band (VB) potentials of the CQDs/FeO
x composite and FeO
x powder are determined using XPS valence spectra. As shown in
Figure 9c, due to the presence of Fe
2O
3, the VB potential of the FeO
x powder was 2.59 eV, which was more positive than E
0(·OH, H
+/H
2O) (2.38 eV vs. NHE). This suggested that the FeO
x powder could oxidize water to generate hydroxyl radical (·OH). However, the conduction band (CB) potential (E
CB = E
VB − E
g) of the FeO
x was determined to be 0.42 eV, which was more positive than the standard electrode potential E
0(O
2, H
+/·O
2H) for superoxide radicals (−0.046 eV vs. NHE). This indicated that the FeO
x powder could not reduce oxygen in water to produce superoxide radical (O
2·–). On the other hand, the introduction of CQDs raised the VB potential of the CQDs/FeO
x composite material to 2.83 eV, enabling better oxidation of water to form photocatalytically active hydroxyl radical. Combining its own band gap (1.40 eV) and the band gap of CQDs (2.14 eV), the CB potential was calculated to be −0.08 eV, which was lower than E
0(O
2, H
+/·O
2H) for superoxide radicals (−0.046 eV vs. NHE). This indicated that the CQDs/FeO
x composite material could reduce oxygen in water to generate photocatalytically active superoxide radical.
The photoluminescence emission profiles of both the CQDs/FeO
x composite material and FeO
x are presented in
Figure 9d. The fluorescence emission intensity exhibited by the CQDs/FeO
x composite material was notably subdued in comparison to that of the FeO
x. This observation implies that the incorporation of CQDs could proficiently curtail the recombination of photogenerated electron-hole pairs, thereby significantly contributing to the enhancement of the photocatalytic degradation efficacy. The enhanced mechanism of the CQDs/FeO
x composite material on the catalytic performance of the FeO
x was also demonstrated through transient photocurrent response (PCR) under visible light irradiation and electrochemical impedance spectra (EIS). As shown in
Figure 9e, under purple light illumination, the photocurrent intensity of the CQDs/FeO
x composite material was approximately 11 times that of the FeO
x without CQDs, indicating that the CQDs/FeO
x composite could achieve a more efficient interface charge transfer and more effective electron-hole pair separation. The lower probability of photogenerated electron-hole recombination resulted in a significant improvement in the photocatalytic degradation performance. Additionally, the Nyquist plot of the CQDs/FeO
x composite displayed a smaller semicircle diameter than that of the FeO
x powder, indicating that the resulting CQDs/FeO
x composite exhibited lower charge transfer resistance than the FeO
x powder. This ensured a more efficient interface charge transfer and more effective electron-hole pair separation, consistent with the photocurrent analysis results (see
Figure 9f).
The impacts of distinct quenching agents (EDTA–2Na, BQ and IPA) on the photodegradation process of methylene blue are elucidated in
Figure 10a,b. Notably, the introduction of EDTA–2Na marginally curtailed the photocatalytic degradation efficacy of the CQDs/FeO
x composite material, yielding a photocatalytic efficiency of 93.44% in comparison to the absence of quenching agents. This observation underscores that photogenerated holes (h+) played a minor role and were not the primary drivers of the photocatalytic activity. In contrast, the incorporation of BQ or IPA substantially impeded the degradation efficiency, yielding photocatalytic efficiencies of 40.75% and 60.15%, respectively, as opposed to the scenario without quenching agents. This phenomenon implies that both superoxide radicals (O
2·–) and hydroxyl radicals (·OH) stood as the predominant active species in the photocatalytic degradation mechanism, with O
2·– playing a more pronounced role. Furthermore, using DMPO as a radical trapping agent, electron spin resonance spectroscopy (ESR) was carried out to study the active oxygen species generated by the CQDs/FeO
x composite and FeO
x. As shown in
Figure 10c–f, the addition of the CQDs/FeO
x composite resulted in strong characteristic peaks of both superoxide radical (O
2·–) and hydroxyl radical (·OH). This indicates that the CQDs/FeO
x composite material could reduce adsorbed O
2 to form superoxide radical (O
2·–) and oxidize adsorbed H
2O to form hydroxyl radical (·OH) under light irradiation. In contrast, under the same test conditions, the FeO
x powder could not generate superoxide radical (O
2·–) effectively, while its signal of hydroxyl radicals was weak.
As shown in
Figure 10g, the possible photocatalytic mechanism of the CQDs/FeO
x composite material was similar to that of the CQDs/TiO
2 [
44] and CQDs/ZnO [
45] composites in our previous report. Upon exposure to visible light, the CQDs/FeO
x composite undergoes a dynamic process: the CQDs become readily excited by photogenerated electrons situated in the conduction band (CB), leaving behind holes in the valence band (VB). This excitation triggers rapid spatial electron transfer between the CQDs and FeO
x particles, effectively suppressing recombination and yielding the enhanced separation of electron-hole pairs. As a result, photogenerated electrons amass in the CB of the CQDs, while the holes populate the VB of FeO
x, with each entity primed for their distinct roles in photocatalytic reactions. Photogenerated holes engage with H
2O to yield a profusion of ·OH radicals, while photogenerated electrons react with O
2, leading to an abundant production of O
2·– radicals. These generated O
2·– and ·OH radicals collectively orchestrate the degradation of diverse organic pollutants, thereby showcasing exceptional prowess in the realm of photocatalytic degradation activity.