To further investigate the synergistic effects of Fe (Ⅲ) and graphene derivatives with varying degrees of oxidation for photocatalysis, commercial titanium dioxide nanoparticles and graphene oxide were employed as precursors to synthesize the catalyst in this study. Graphene oxygenated derivatives and Fe (Ⅲ)-modified titanium dioxide photocatalysts with different oxidation degrees were prepared using a simple one-step solvothermal method. The results demonstrated that the photocatalytic performance in degrading rhodamine B and sulfamethoxazole was enhanced with an increase in the oxidation degrees of graphene materials. Through the combined action of delocalized conjugated π electrons as electron transfer mediators, Fe (Ⅲ) as an electron trap, and photosensitization reactions, titanium dioxide exhibited exceptional photocatalytic properties with the assistance of graphene derivatives and Fe (Ⅲ) co-catalysts in the degradation of organic compounds.

  • We developed a distinctive and straightforward method for fabricating graphene oxide and Fe(III) co-modified titanium dioxide catalysts.

  • The quantity of oxygen-containing functional groups on the surface of graphene oxide precursors was controlled through thermal reduction.

  • The synergistic impact of graphene derivatives and Fe (III) dual co-catalysts was further enhanced.

In recent years, persistent organic pollutants (POPs) and antibiotics have become a growing focus of attention. Emerging contamination (EC) such as persistent organic pollutants (POPs), pharmaceuticals and personal care products (PPCPs) enter the environment through multiple pathways and place a huge burden on the environment (Katsoyiannis & Samara 2004; Yanei et al. 2023; Die Ling et al. 2024). Research shows that 15% of persistent organic dyes in the wastewater produced by the textile industry are discharged into the water without treatment and 30% of antibiotics are discharged into the environment without being absorbed and utilized by animals and plants (Karthikeyan & Meyer 2006; Channei et al. 2014). Unfortunately, these pollutants are difficult to degrade by traditional biological treatment methods and cause further pressure on the surroundings (Guo Dong 2019; Chen et al. 2023). Thus, it is necessary to find a more efficient treatment process (Kurniawan et al. 2020).

The development of photocatalytic oxidation processes utilizing highly reactive oxygen species (ROS) such as H2O2, ·OH, and ·OOH for the efficient treatment of wastewater has attracted widespread attention in recent years. Photocatalytic oxidation, a green, mild and environmental-friendly technology, has been one of the important ways to control environmental problems in recent years (Fujishima et al. 2000; Anpo & Kamat 2010; Nosaka & Nosaka 2013). Photocatalytic oxidation processes can degrade nearly all of the organic pollutants in the wastewater (Michael & Henderson 2011). Of all of the photocatalysts, TiO2 is considered to be one of the most promising catalysts due to its good chemical stability, biocompatibility, availability and low cost (Drunka et al. 2015). However, anatase TiO2 has a narrow light absorbance range (<380 nm) because of the large band gap of 3.2 eV. The high recombination efficiency of photogenerated electrons and hole has a negative effect on the formation of ROS (Asahi et al. 2001; Jin & Zhen 2002; Christian et al. 2014). Limited visible light utilization and low electron–hole separation efficiency are the main disadvantages that hinder its further application.

In order to improve the photocatalytic activity of TiO2, a series of feasible approaches mainly including doping and surface sensitization have been proposed (Ruohang et al. 2023; Zhifeng et al. 2023). Among them, the surface modification of TiO2 by Fe (Ⅲ) and graphene have been found to be of particular interest because of their synergistic effect as electron co-catalysts. As a common transition metal, Fe (Ⅲ) has been proven to be a very effective co-catalyst. On one hand, Fe (Ⅲ) doped in TiO2 lattice changes its crystalline shape, which improves the photocatalytic efficiency and promotes the utilization of visible light by shortening the band gap and broadening the light absorption range. On the other hand, Fe3+/Fe2+ (0.771 V) has more positive potential than the conduction band of TiO2. It generates electron traps on the semiconductor surface. Meanwhile, Fe (Ⅱ) can reduce oxygen rapidly by a possible multi-electron reduction mechanism (4Fe2+ + O2 + 4H+→ 4Fe3+ + 2H2O or 4Fe2+ + O2 + 2H2O → 4Fe3+ + 2OH), which eventuates the efficient transfer of photogenerated electrons with Fe (Ⅲ) surfaced modification of the catalyst (Li et al. 2008; Hemmati Borji et al. 2014; Yu et al. 2015; Shufang et al. 2023). However, the electron migration capability is restricted because the contact between the Fe (Ⅲ) co-catalyst and the catalyst is very limited, while graphene and its derivatives have a large specific surface area. The large number of contact sites between graphene derivatives and catalysts will further accelerate the electron migration process (Yu et al. 2015). In recent years, the field of two-dimensional material graphene nanocomposites has developed rapidly due to the highly conjugated hexagonal honeycomb structure (Zhao & Yang 2019), which has a wide range of applications in photocatalysis. Graphene has a large specific surface area, photochemical stability and adsorption capacity. The zero band gap of graphene allows photogenerated electrons to be excited at the Fermi energy level under visible light irradiation, thus broadening the light absorption range. The delocalized conjugated π electron system of graphene can be used as a mediator for photogenerated electron transfer to improve the separation efficiency of semiconductor photogenerated electron–hole pairs (Neto et al. 2009; Mak et al. 2010; Bo et al. 2018; Zhang et al. 2019; Shufang et al. 2023). It has been widely demonstrated that the surface modification of graphene derivatives greatly improves the photocatalytic performance of various photocatalysts. In numerous studies by scholars, however, rGO is often used as a co-catalyst, because the synthesis temperature of graphene-based photocatalysts is often higher than the thermal reduction temperature of graphene oxide (GO) in numerous preparation methods (Shen et al. 2011). In fact, the hydrophilic capacity of GO and rGO differ greatly due to the different number of oxygen-containing functional groups, which bring different degrees of influence on the process of assisting photocatalysts to catalyze organic compounds. The effect of different oxidation degrees of graphene derivatives on photocatalysis has not been mentioned.

Here, graphene derivatives and Fe-modified titanium dioxide with different oxidation degrees are successfully prepared by a simple one-step solvothermal synthesis method, where titanium dioxide nanoparticles and GO are used as precursors. The high-temperature and high-pressure conditions of the solvothermal method not only combine GO with TiO2 and Fe (Ⅲ) easily but also have the advantage of being industrialized. The varying exothermic degradation of oxygen-containing groups in GO occurs under 150–300 °C (Yap et al. 2023). Thus, various types of graphene oxygenated derivatives can be prepared by thermal reduction with varying temperatures. The prepared catalysts showed significantly better performance than TiO2 in experiments for the degradation of rhodamine B (RhB) and sulfamethadiazole (SMX). More importantly, with the increase of oxygen-containing functional groups, it was found that adsorption and sensitized photolysis have a non-negligible role in promoting the photocatalytic performance of the materials. In this paper, the relationship between the sensitized photolysis and the synergistic effect of graphene and Fe (Ⅲ) co-catalysts will be discussed in depth on the basis of existing studies.

Materials

Nano titanium dioxide, Fe(NO3)3·9H2O, polyvinyl pyrrolidone (M ≈ 8,000, K = 16 ∼ 18) and absolute ethanol were purchased from Aladdin. Multilayer GO was obtained from Shenzhen, China. Rhodamine B (RhB) and sulfamethoxazole (SMX) as degradation substrates were purchased from Macklin. A hydrochloric acid solution was used to regulate pH. All the chemicals were analytical grade and all the solutions were made using deionized water.

Synthesis of catalysts

During the synthetic process, TiO2 was used as a precursor to prepare graphene-based photocatalytic by one-step solvothermal method. 0.5000 g GO, 0.5000 g TiO2, 2.0 g polyvinyl pyrrolidone and 5.0 mL Fe3+ solution (100 mg/L, pH = 2) were dispersed in 80 mL ethanol/water (1:3) solution by using ultrasonic (360 W, 40 kHz) for 30 min. The gray suspension was synthesized by polytetrafluoroethylene (PTFE)-lined high-pressure reactor in the container at 105 °C for 24 h. The product was washed with deionized water, filtered and dried at 60 °C, and the GO and Fe (Ⅲ) modified TiO2 labeled as GOFT-105 was prepared. the catalysts GOFT-150, rGOFT-180, rGOFT-210 and rGOFT-270 were obtained by calcining GOFT-105 at 150, 180, 210 and 270 °C for 1 h, respectively. The abbreviations ‘F’ and ‘T’ are defined as Fe (Ⅲ) and TiO2 load on the substrate GO or reduced graphene oxide (rGO).

Characterization

Scanning electron microscopy (SEM) images of the detail morphology of materials were captured by a microscope (MIRA LMS, TESCAN, Czech). The Fourier transform infrared (FTIR) spectra of the samples with wavelengths ranging from 500 to 4,000 cm−1 for analyzing the information on oxygen-containing functional groups were obtained by Plastic Analyzer (Shimadzu, Japan). The thermogravimetric data of the catalyst were obtained by thermogravimetric analysis (TG, SDT Q600, America). The information on the structural integrity of sp2 in graphene derivative was obtained by Raman spectroscopy (alpha300R, WITec, Germany) by using a 532 nm, 6.0 mW laser. An X-ray photoelectron spectroscopy (XPS, Nexsa, Thermo Scientific, America) was applied to study the chemical valences and the oxidation degree of graphene derivative. UV-vis diffuse reflectance spectra ranging from 200 to 800 nm for calculating the band gap energy of catalysts were taken from a UV-vis spectrophotometer (PE Lambda 950, PERKINELMER, America). The electron paramagnetic resonance (EPR) spectrum of the material under ultraviolet light was obtained by the EPR test (Bruker EMX PLUS, Germany).

Photocatalytic performance

Photocatalysts maintained at 0.2 g/L concentration were first dispersed in deionized water by ultrasound and then tested in a 500 mL beaker with 200 mL organic wastewater with the concentration of 15 mg/L RhB and 10 mg/L SMX, respectively, under the stirring of the magnetic stirrer. The UV-light degradation was carried out by using a UV-light lamp (30 W, 253.7 nm, ZW30S19W, Guangzhou, China) and the simulated sunlight degradation was carried out by xenon lamp (300 W, CEL-HXF300, Beijing, China). Samples were filtered with the needle filter (0.45 μm, Φ = 13 mm) and the absorbance change was measured by UV-vis spectrophotometer (UV759, YOKE, Shanghai, China) at the wavelength of 554 nm (RhB) and 257 nm (SMX). The degradation efficiency was expressed by:
The kinetics was expressed as:
The adsorption capacity of catalyst adsorbs RhB's-simulated-contaminated water with time variation was calculated by:
where C0 and C are substance concentrations at an initial time and after reacting for t min, V is the volume of the solution, m is the mass of catalysts, k is the apparent rate constant and qe is the adsorption capacity. For the control group (Figure 1), graphene derivatives (GO-105, GO-180) were treated in the same way, directly thermally reduced with GO and the Fe-modified titanium dioxide (Fe/TiO2) remaining after calcination of the catalyst GOFT-105 at 500 °C for 1 h was used for control experiments.
Figure 1

Control group material design process.

Figure 1

Control group material design process.

Close modal

Structural characterization and analysis

The SEM image in Figure 2 reveals that both cubic and spherical TiO2 are present on the surface of the graphene structure. Additionally, the protrusions on the surface of graphene wrinkles may be Fe2O3 and FeO, which was confirmed through XPS analysis. The diameter of the titanium dioxide particles ranges from 50 to 150 nm, with a small number of TiO2 particles exhibiting clear boundaries and measuring approximately 40 ∼ 60 nm. This observation is attributed to the partial dissolution of TiO2 in the liquid phase under solvothermal conditions, leading to the formation of ionic clusters that subsequently nucleate and crystallize into grains. Both TiO2 and Fe (Ⅲ) are dispersedly loaded onto the surface of folded GO. The GOFT catalyst folds to form a lumpy particle with a particle size approximately 5–20 μm (Figure 2(f)). The presence of a wrinkled structure significantly increases the specific surface area, providing more active adsorption sites for reactions.
Figure 2

SEM image of GOFT-105 (a–d) and particle size distribution statistics graph of titanium dioxide (e) and GOFT photocatalyst (f).

Figure 2

SEM image of GOFT-105 (a–d) and particle size distribution statistics graph of titanium dioxide (e) and GOFT photocatalyst (f).

Close modal
In the FTIR analysis (Figure 3(a)), numerous absorption peaks were observed, including the O–H bond at 2,400 to 3,600 cm−1, as well as peaks at 1,614 and 1,416 cm−1, corresponding to the C = O bond at 1,728 and 1,039 cm−1, and the C–O bonds at 1,374 cm−1 in −COOH. Additionally, epoxy bonds at 1,270 cm−1 and tertiary hydroxyl C–O bonds at 1,168 cm−1 were identified in the GO-105 sample. These peaks are indicative of oxygen-containing functional groups such as −OH, −COOH, and -C = O, as well as interlayer molecular water (Miaomiao et al. 2021). The above-mentioned peaks were notably weakened or disappeared altogether in rGO-180, with only two weak absorption peaks appearing at 1,698 and 1,533 cm−1. Both of these peaks correspond to the expansion and vibration of C = C bonds, indicating that the majority of oxygen-containing functional groups present in GO were removed during the reduction process (Gang et al. 2020; Miaomiao et al. 2021). When the temperature exceeds 160 °C, in reality, the hexagonal honeycomb structure of GO was restored to some extent, thus GO was reduced to rGO (Yap et al. 2023). In the catalysts prepared at varying temperatures, a consistent trend was observed: as the reduction temperature increased, the absorption peaks weakened or disappeared altogether. Additionally, at 1,500 to 1,700 cm−1, the shift of the absorption peaks of the C = C bond was found to be related to the recovery of the sp2 hybrid structure, leading to an enhanced vibrational coupling effect of the C = C bond.
Figure 3

FTIR spectra of GO-105, rGO-180, GOFT-105, GOFT-150, rGOFT-180, rGOFT-210 and rGOFT-270 (a); thermogravimetric curve of GOFT-105 (b) and its first derivative (c).

Figure 3

FTIR spectra of GO-105, rGO-180, GOFT-105, GOFT-150, rGOFT-180, rGOFT-210 and rGOFT-270 (a); thermogravimetric curve of GOFT-105 (b) and its first derivative (c).

Close modal

Thermogravimetric analysis of GOFT-105 in a simulated preparation environment reveals two peaks in the first derivative of the thermogravimetric curve (Figure 3(c)). The mass loss observed between 60 and 130 °C can be attributed to the evaporation of molecular water between GO layers, while that observed between 170 and 250 °C is mainly due to the pyrolysis of oxygen-containing functional groups, resulting in the conversion of GO into rGO (Yap et al. 2023). As the calcination temperature increases, the number of oxygen-containing functional groups on the surface of each sample's graphene derivatives gradually decreases, which is consistent with the results obtained from infrared spectroscopy.

In the catalyst, the full XPS spectra (Figure 4(a)) revealed the presence of Ti 2p, O 1 s, Fe 2p, N 1 s, and C 1 s. In the energy range of 700–735 eV (Figure 4(b)), characteristic peaks corresponding to Fe 2p1/2 (711.5 eV) and Fe 2p3/2 (725.1 eV), as well as satellite peaks were observed, indicating the presence of Fe (Ⅲ) (Channei et al. 2014; Yu et al. 2015). This was attributed to the formation of Ti–O–Fe bonds, with Fe3+ replacing Ti4+ and the deposition of Fe2O3 on the surface. Additionally, peak fitting analysis identified characteristic peaks of Fe2+ at 709.6 and 723.4 eV, suggesting the possible existence of FeO under high temperature and pressure (He et al. 2005; Thanh et al. 2019). The characteristic peaks of C 1 s (Figure 4(c) and 4(d)) in GOFT-105 and rGOFT-180 revealed the presence of various bonds, including C = C bond, C–C bond, and C–H bond (284.8 eV), C–O bond (286.1 eV), C = O bond (288.0 eV), and O = C–OH group (288.6 eV) (Qiu et al. 2015; Zou 2021). It is evident from the figure that the number of oxygen-containing functional groups on the surface of GOFT-105 decreased when it was converted into rGOFT-180. This is apparent from the difference in peak area in the figure of C 1 s fine spectra.
Figure 4

Full XPS spectra of catalyst (a), Fe 2p fine spectra (b) and C 1s fine spectra (c, d) of GOFT-105 and rGOFT-180; Raman spectra of GOFT-105 and rGOFT-180 (e) and histogram (f).

Figure 4

Full XPS spectra of catalyst (a), Fe 2p fine spectra (b) and C 1s fine spectra (c, d) of GOFT-105 and rGOFT-180; Raman spectra of GOFT-105 and rGOFT-180 (e) and histogram (f).

Close modal

The Raman spectra (Figure 4(e)) exhibited five characteristic peaks at 150, 201, 391, 510 and 632 cm−1, which were assigned to the Eg, Eg, B1g, A1g + B1g and Eg modes of the anatase phase titanium dioxide (Gupta et al. 2010). The inset of the figure displayed the Raman spectra of GOFT-105 and rGOFT-180, which showed the characteristic D band at 1,342 cm–1 and G band at 1,591 cm–1. It is well known that the relative intensity of the D band and the G band is indicative of the proportions of sp3 C atom and sp2 C atom in graphene (Yan et al. 2022). The thermal decomposition of oxygen-containing functional groups converts GO into rGO, resulting in the restoration of sp2 domains. However, both samples exhibit similar ratios (Figure 4(f)), indicating the occurrence of carbon vacancies (VC) formation, which introduces additional sp3 defects (Shen et al. 2013).

The band gap of the photocatalysts was determined using the equation derived from Tauc Equation and Beer–Lambert's Law (Davis 1970):
The UV-vis spectra (Figure 5) show that there was a significant red shift in the absorption range when graphene derivatives and Fe (Ⅲ) co-catalysts were introduced for modification, indicating a reduced band gap of TiO2. The band gaps of the various graphene derivatives modified materials, treated at 105, 150, 180, 210 and 270 °C, were calculated to be 2.82, 2.61, 2.85, 2.68 and 2.69 eV, respectively. Notably, the photocatalyst treated at 150 °C displayed the lowest band gap energy. Applying the formula:
the optical absorption threshold was determined to be 470 nm. This calculation suggests an enhanced photocatalytic performance and improved utilization of sunlight for the material.
Figure 5

UV-vis spectra (a) and band gap energy (b) of Fe/TiO2, GOFT-105, GOFT-150, rGOFT-180, rGOFT-210 and rGOFT-270.

Figure 5

UV-vis spectra (a) and band gap energy (b) of Fe/TiO2, GOFT-105, GOFT-150, rGOFT-180, rGOFT-210 and rGOFT-270.

Close modal

Photocatalytic performance

The objective of this study was to assess the efficacy of the samples as photocatalysts for the degradation of RhB and SMX in aqueous solutions under UV-light and visible light irradiation. Whether it was RhB or SMX (Figure 6(a)–6(c)), the catalysts with graphene derivatives co-catalyst had much stronger degradation performance than single Fe/TiO2. The sensitization modification of graphene derivatives allowed TiO2 to harness a greater amount of visible light and the shortest band gap material GOFT-150 had higher visible light utilization efficiency compared with other catalysts (Figure 6(c)). Additionally, it was observed that the more oxidized materials exhibited heightened catalytic activity in the degradation of RhB and SMX, as evidenced by the dark adsorption of RhB within the initial 30 min. It is important to highlight that graphene derivatives themselves have the ability to sensitize the photolysis of organic matter. In the control group, GO-105 and GO-180, which had achieved adsorption equilibrium, were employed for the degradation of RhB at the same concentration (0.1 g/L) as the experimental group. The findings revealed that the more oxidized graphene derivatives exhibited greater efficacy in sensitizing the photolysis of RhB (Figure 6(d)). It can be seen from the adsorption curve that the catalyst had a fast adsorption speed and reached the equilibrium in about 30 min (Figure 6(f)), thus the pseudo-first-order kinetic model can well describe the degradation process of the substrate. The rate constants for RhB degradation by all catalysts under UV-light ranged from 0.117 to 0.188 min−1, which was 3.0 to 4.8 times higher than that of Fe/TiO2. However, the degradation mechanism of SMX is more intricate. Currently, the kinetic process of SMX degradation reaction is not well established, hence it has not been calculated. GOFT-105 exhibits superior photocatalytic oxidation performance due to its excellent adsorption capability and efficient electron mobility. However, after five cycles of photocatalytic experiments (Figure 6(e)), the degradation efficiency of GOFT-105 was only 72.0%, while rGOFT-180 achieved a higher efficiency of 84.4%. The figure revealed a reduction in surface hydroxyl groups of the graphene derivatives due to excessive chemical adsorption during catalyst usage. This implies that an excess of oxygen-containing functional groups on the material leads to increased chemical adsorption of organic matter, which is why GO-based catalysts are more prone to deactivation (Li et al. 1990). Comparison of the infrared spectrum analysis of GOFT-105 after the adsorption and degradation processes with the spectroscopy of the initial catalyst and substrate revealed the vanishing of the characteristic peak of RhB after the degradation process, demonstrating that most of the substrates are removed and verifying the regeneration of the adsorption sites of catalysts (Figure 6(g)).
Figure 6

Photocatalysts degraded 15 mg/L RhB (a) and 10 mg/L SMX (b) under UV-light; photocatalysts degraded 15 mg/L RhB under visible light (c); graphene derivatives degraded 15 mg/L RhB under UV-light irradiation (d); five cycles of photocatalysis (e); adsorption curve of photocatalyst under the same condition (f); IR spectra of the catalyst GOFT-105 after adsorption and degradation process (g).

Figure 6

Photocatalysts degraded 15 mg/L RhB (a) and 10 mg/L SMX (b) under UV-light; photocatalysts degraded 15 mg/L RhB under visible light (c); graphene derivatives degraded 15 mg/L RhB under UV-light irradiation (d); five cycles of photocatalysis (e); adsorption curve of photocatalyst under the same condition (f); IR spectra of the catalyst GOFT-105 after adsorption and degradation process (g).

Close modal
Figure 7

Electron paramagnetic resonance tests of ·OH (a) and (b) in GOFT-105 sample; schematic diagram illustrating the enhanced photocatalytic performance of catalyst (c).

Figure 7

Electron paramagnetic resonance tests of ·OH (a) and (b) in GOFT-105 sample; schematic diagram illustrating the enhanced photocatalytic performance of catalyst (c).

Close modal

Mechanism analysis

In experiments involving the photocatalytic degradation of typical persistent organic pollutants and antibiotics, this type of catalyst demonstrated superior photocatalytic performance when compared to single Fe-modified titanium dioxide. This was attributed to the synergistic effect of delocalized conjugated π electron and Fe (III) electron traps on the surface of graphene derivatives, providing a good transport channel for photogenerated electrons and inhibiting the recombination of photogenerated electron-hole pairs. EPR spectra exhibited the characteristic peaks of 5,5-dimethyl-1-pyrroline N-oxide (DMPO)·OH and DMPO- after 5 min of ultraviolet radiation. These major radicals are involved in photocatalytic oxidation reactions. Specifically, the main mechanism involves graphene derivatives capturing photogenerated electrons from the surface of TiO2, serving as electronic mediators to transfer electrons from the capture site to Fe (III) clusters. Oxygen is rapidly reduced to and ·OOH on the surfaces of graphene derivatives and Fe (III) clusters, while water is swiftly oxidized to ·OH on the surface of TiO2 (Figure 7).
Figure 8

Schematic diagram of photocatalytic and photosensitization co-degradation of pollutants.

Figure 8

Schematic diagram of photocatalytic and photosensitization co-degradation of pollutants.

Close modal

Additionally, an increase in oxidation degree led to an increase in the photocatalytic reaction rate constant. Therefore, oxygen-containing functional groups on the surface of graphene derivatives play a crucial role. On one hand, this is because these functional groups aid in the connection between TiO2 and graphene derivatives. The πd electron coupling facilitates the rapid transport of photogenerated electrons between graphene derivatives and TiO2, effectively inhibiting the recombination of photogenerated electron-hole pairs in TiO2, resulting in a high-performance photocatalyst. On the other hand, an increase in oxygen-containing functional groups enhances the material's hydrophilicity, improving the chemical adsorption of pollutants in water and increasing the bonding ability with various pollutant molecules. Furthermore, graphene derivatives act as photosensitizers to sensitize photolysis, with n-type semiconductor GO exhibiting a more potent sensitization effect on pollutants than p-type semiconductor rGO (Figure 8). This sensitization effect further improves the photocatalytic efficiency of graphene derivatives.

Through a comprehensive analysis of morphological and chemical characterization results, it is evident that the GO precursor was effectively dispersed using polyvinyl pyrrolidone (PVP) dispersant, and titanium dioxide catalysts modified with graphene derivatives containing Fe (III) and varying degrees of oxidation were successfully prepared. The formation of pn or nn heterojunctions between graphene derivatives and TiO2 leads to alterations in the catalyst's band structure, resulting in a narrower band gap and an expanded light absorption range for the material. This study demonstrates that photocatalysts modified with graphene derivatives exhibiting higher oxidation levels exhibit superior photocatalytic performance. The synergistic interplay of electron transport between these graphene derivatives and Fe (III), as well as the sensitization photocatalytic effect of the graphene derivatives themselves, collectively contribute to the heightened efficiency of photocatalysis. Additionally, the synergistic impact of graphene derivatives and Fe (III) dual co-catalysts was further amplified.

The authors gratefully acknowledge the financial support provided by Hainan Province Key Scientific Research Project (ZDYF2021GXJS026); National Natural Science Foundation of China (Grant No. 52360002). We also appreciate the editors' valuable comments very much, which are helpful to improve the quality of our present study.

All relevant data are included in the paper or its Supplementary Information.

The authors declare there is no conflict.

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