1. Introduction
Water pollutants have attracted considerable attention from all levels of society because of the increasing challenges in environmental concerns and energy demands [1]. Harmful pollutants, such as antibiotics, dyes and heavy metals, pollute the water significantly and threaten human health. Ciprofloxacin (CIP), a commonly used antibiotic in all aspects of life [2], can have a serious impact on the ecological environment balance [3]. To date, several strategies, including electro-Fenton [4], biological degradation [5], adsorption [6], membrane filtration [7] and photocatalytic degradation [8], have been employed to remove contaminants. Among them, photocatalysis has attracted more attention for the degradation of antibiotics [9]. Due to the cost-effectiveness and excellent stability, photocatalysts are considered ideal solids for water purification [10]. However, traditional semiconductor-based photocatalysts exhibit poor photoactivity due to the low utilization of solar energy and rapid recombination of photo-induced electrons and holes, consequently, their application in the removal of organic pollutants is restricted [11,12].
Graphitic carbon nitride (g-C3N4) has received great attention due to its unique electronic structure, high thermal and chemical stability, high hardness, low density, good biological compatibility and high wear resistance [13,14,15]. However, poor solar energy utilization, low specific surface area and low number of active sites [16] are the main factors explaining the low photocatalytic performance of g-C3N4 [17]. To improve the photocatalytic performance of g-C3N4, great effort has been made to modify the structure and texture by means of various strategies, such as elements doping [18,19], creation of porosity [20,21], noble metals deposition [21,22], loading metal nanoparticles [23,24] and construction of semiconductor heterojunctions [25,26,27]. Among numerous experimental procedures, semiconductor coupling has proven an excellent approach for promoting charge separation and photocatalytic performance [28]. One of the most important semiconductor materials is cerium oxide (CeO2), which is used in a wide range of industrial applications, such as catalytic reactions, solar and fuel cells. This is due to its appealing low cost, high chemical stability, high oxygen storage capacity and strong advantages [29,30,31,32,33]. In addition, CeO2 is an excellent photocatalyst due to the narrow band gap, and absorption of visible light [34,35]. Therefore, CeO2/semiconductor heterojunction formation not only improves conversion rates of light energy, but can accelerate the separation of electrons and holes, with a positive impact on the photocatalytic activity [36].
Kaolin, a nonmetal phyllosilicate clay mineral, is mainly composed of layers of silica tetrahedra and alumina octahedra, with good hydrophilic and adsorption properties [37,38,39,40]. Due to the large specific surface area and pore volume, it exhibits high adsorption capacity of organic compounds. As a result, it is often used as a carrier for photocatalytic and adsorption materials. Over the last few decades, kaolin/TiO2, kaolin/CeO2, CeO2/g-C3N4 [41,42] and kaolin/g-C3N4 composites have been investigated [43,44,45]. However, the construction of ternary kaolin/CeO2/g-C3N4 heterojunction photocatalyst is yet to be reported. Due to the fact that kaolin has unique structural and adsorption properties, the combined photocatalyst should further improve the light utilization and accelerate the interfacial charge transfer. Therefore, it would be an excellent strategy to combine the g-C3N4/CeO2 heterostructure with a natural mineral, such as kaolinite, to synthesize a ternary photocatalyst with enhanced photocatalytic activity, since both adsorption capacity and adsorption of visible light can be increased [29,46,47].
Herein, a novel ternary kaolin/CeO2/g-C3N4 heterostructure was fabricated via a facile sol-gel method followed by a mild hydrothermal treatment. The structure and morphology of kaolin/CeO2/g-C3N4 heterostructure were characterized systematically by TEM, XRD, EDS, N2 Physisorption, XPS, Brunauer-Emmett-Teller (BET) theory, SEM, electrochemical impedance spectroscopy (EIS), EPR and UV-Vis diffuse reflectance spectra (DRS). The synthesized kaolin/CeO2/g-C3N4 heterostructure exhibited outstanding photocatalytic activity towards CIP under visible-light irradiation. Hence, 90% CIP degradation efficiency was obtained within 150 min, which was 2-folds higher than that of pristine g-C3N4. The reasons for enhanced photocatalytic activity originated from improved light harvesting and enhanced separation and transfer efficiency. Based on the obtained experimental results, the mechanism of photocatalytic degradation over kaolin/CeO2/g-C3N4 composite was also proposed. 2. Experimental 2.1. Materials The purified kaolin was obtained from Jingdezhen, in the eastern province of Jiangxi province, China. NaOH, Ce(NO3)3•6H2O, ciprofloxacin, melamine, urea, ethanol and nitric acid were purchased from Aladdin industries and were of analytical grade. 2.2. Preparation of g-C3N4
The g-C3N4 powder was prepared according to previous work [48]. In a typical procedure, urea (15 g) and dicyandiamide (15 g) were mixed into a covered alumina crucible and heated at 550 °C (heating rate of 5 °C/min) for 4 h. The resulting yellow solid powder was collected for further use.
2.3. Preparation of Kaolin/CeO2 Composite Ce(NO3)3•6H2O (1.305 g) and NaOH (14.400 g) were dissolved in distilled water (60 mL) under magnetic stirring for 2 h. Then, the homogeneous solution was transferred to a 100 mL Teflon-lined stainless steels autoclave and heated at 180 °C for 24 h. Subsequently, the autoclave was naturally cooled to room temperature. The resulting precipitate was washed three times with distilled water and ethanol. The product was added to deionized water (60 mL) and magnetically stirred for 2 h producing suspended solution A. Kaolin (1.0 g) was immersed in ethanol (30 mL), magnetically stirred for 30 min and sonicated for 2 h producing solution B. Then, suspended solution A was slowly added to suspension B with stirring for 12 h. The obtained product kaolin/CeO2 was dried in an oven at 80 °C for 12 h and heated at 450 °C (heating rate of 5 °C/min) for 3 h in a muffle furnace. For comparison, CeO2 was synthesized using a similar method without kaolin. 2.4. Preparation of Kaolin/CeO2/g-C3N4 Composite A certain amount of the kaolin/CeO2 composite was dispersed in ethanol solution and stirred for 12 h, (solution A). Separately, a certain amount of g-C3N4 powder was dispersed in ethanol solution and stirred for at least 8 h, (solution B). Then, solution B was added dropwise to solution A and stirred continuously for 1 h, (solution C). The solution C was continuously stirred for 24 h at room temperature. The obtained suspension was centrifuged and the obtained solid dried in an oven at 60 °C for 12 h. The dried sample was ground and heated to 550 °C (heating rate of 5 °C/min) for 4 h in a muffle furnace. The obtained sample was a kaolin/CeO2/g-C3N4 composite. 2.5. Characterization X-ray diffraction (XRD) was performed on a Bruker D8 Advance (Cu-Kα source, λ = 1.5418 Å, 45 KV, and 40 mA). The samples were scanned within the range of 5° to 80° 2θ with a scanning speed of 7°/min. X-ray photoelectron spectroscopy (XPS, Al Ka, hv = 1486.7 eV, reference C 1 s binding energy of 284.8 eV) was used to analyze the elemental composition and chemical state at the sample surface. A Lambd950 spectrophotometer (Perkin Elmer, Costa Mesa, CA, USA) was used to record the UV-Vis spectra between 200 and 800 nm. UV–Vis diffuse reflectance spectra were registered on a Hitachi-3900H spectrophotometer (Tokyo, Japan). SEM images were recorded on a S-4800 scanning electron microscope equipped with a 5.0 KV energy dispersive spectrometer produced by Hitachi high-tech Co. Ltd. (Tokyo, Japan) TEM and HRTEM images were collected on a field emission transmission electron microscope and JEM-3010 electron microscope, respectively, produced by JEOL (Tokyo, Japan). The EPR test was carried out on SPINSCAN X (ADANI Company, Minsk, Belarus). The N2 physisorption was performed on a JW-BK (JWGB, Beijing, China) surface area and pore size analyzer at the temperature of liquid nitrogen (77 K). The specific surface area was calculated according to the Brunauer-Emmett-Teller (BET) theory while the pore size distribution was assessed by applying the Barrett-Joyner-Halenda (BJH) model to the isotherm adsorption branch. 2.6. Photocatalytic Activity The photocatalytic activity of the as-prepared composites was evaluated in the degradation of CIP using a 500 W Xenon lamp with a UV-cutoff filter (λ > 420 nm). Prior to each experiment, 50 mg catalyst were dispersed in 50 mL of CIP solution (20 mg/L). Before irradiation, the suspension was stirred for 60 min in the dark to reach the adsorption-desorption equilibrium. Then, the reaction was initiated by turning on the irradiation. Samples of 5 mL were taken off every 30 min and centrifuged to remove the photocatalyst before analysis by UV-vis spectrophotometry. The concentration of CIP was determined by monitoring the change in absorbance at 273 nm. 3. Results and Discussion 3.1. Physicochemical Properties
The crystalline structure of the as-prepared samples was analyzed by XRD. As shown in Figure 1a, the diffractogram of kaolin displays diffraction peaks at 24.98°, 38.54° and 62.46°, which were assigned to the (002), (202) and (060) planes, respectively, in line with the reference card of the standard pattern (JCPDS No.14-0164). Two distinct diffraction peaks at 12.74° and 27.60° in the diffractogram of pure g-C3N4 corresponded to the (002) and (100) crystal planes of g-C3N4, according the standard card of JCPDS No. 87-1526. The diffraction peaks of pure CeO2 were distinctly observed in the corresponding XRD pattern (JCPDS No.43-1002). The XRD pattern of kaolin/CeO2/g-C3N4 composite displayed the characteristic peaks of g-C3N4 and CeO2 at 27.64° and at 28.4°, respectively, while the characteristic peaks of kaolin were not visible due to the loss of structural ordering and dehydroxylation during the calcination. In addition, compared with the kaolin/CeO2/g-C3N4 sample, the (111) diffraction peaks of CeO2 and the (110) diffraction peaks of g-C3N4 are slightly shifted (Figure 1b), which indicates a lattice distortion in the kaolin/CeO2/g-C3N4 composite [49].
XPS measurements were performed to investigate the elemental composition and chemical states on the surface of as-prepared samples. The survey XPS spectrum of the kaolin/CeO2/g-C3N4 nanocomposite is depicted in Figure 2a and confirms the existence of Ce, O, C, N, Al and Si elements. As shown in Figure 2b, the Ce 3d high resolution XPS spectrum displays peaks at 898.2 and 916.5 eV, which are ascribed to Ce(IV) 3d5/2 and Ce(IV) 3d3/2, respectively, whereas peaks at 882.4 and 888.8 eV are attributed to Ce(III) 3d5/2, and peaks at 900.8 and 907.3 eV are ascribed to Ce(III) 3d3/2. In Figure 2c, the signal of O 1s was fitted with two peaks centered at 529.3 and 532.4 eV, corresponding to Ce-O bond and the absorbed oxygen on the CeO2 surface, respectively. Figure 2d shows the spectrum of C 1 s, which displays two peaks at 284.8 and 288.2 eV attributed to C-NH2 and N-C=N groups, respectively, in g-C3N4. As shown in Figure 2e, depicting the N 1 s high resolution XPS spectrum, there are three distinct peaks at 398.6, 399.6 and 401.0 eV, which were ascribed to sp2 –bonded nitrogen (N-C=N), tertiary nitrogen (N-(C)3) and N-H side groups, respectively. The peak at 404.4 eV might be caused by the charge effect. Theoretically, Si and Al elements may originate from the kaolin. Hence, the XPS results confirmed the successful coupling of kaolin and CeO2 with g-C3N4.
EPR was used to investigate the structural defects in kaolin/CeO2/g-C3N4 composite and mono component samples. As shown in Figure 2f, no signal was detected in CeO2, suggesting the absence of defects in CeO2. However, signals were detected for g-C3N4, kaolin and kaolin/CeO2/g-C3N4 composite. In addition, it was noticed that the signal intensity of kaolin/CeO2/g-C3N4 was higher than that of g-C3N4, indicating that the kaolin/CeO2/g-C3N4 composite should exhibit improved catalytic activity, Therefore, the presence of g-C3N4 had a significant influence on the reactive species because of the changed transfer pathway of charges.
SEM and TEM were employed to investigate the morphology and structure of the as-prepared samples. As shown in Figure 3a,b, a 3D “sandwich” structure was formed by the hydrogen ions functionalized process in the kaolin/CeO2/g-C3N4 composite. The CeO2 displays a nanorod morphology, the nanorods having diameters of 50–80 nm. The 2D nanosheet morphology of g-C3N4 with a wrinkled structure was obtained in the thermal polymerization process. Kaolin had a bulk morphology due to the amorphization and aggregation during the thermal treatment. The kaolin/CeO2/g-C3N4 composite was further investigated by HRTEM. As shown in Figure 3c,d, a lattice spacing of 0.31 nm was observed, which corresponds to the (1-1-1) plane of CeO2. The lattice spacing of g-C3N4 and kaolin was not clearly observed due to poor crystallinity. Energy dispersive spectrometer (EDS) and elemental mapping showed that C, N, O, Si and Ce were uniformly distributed at the surface of the heterostructure (Figure S1).
UV-vis diffuse reflectance spectroscopy was used to study the optical properties of g-C3N4, CeO2, CeO2/g-C3N4 and kaolin/CeO2/g-C3N4 samples, and the spectra are illustrated in Figure 4a.
The spectrum of kaolin/CeO2/g-C3N4 composite displays a peak with maximum at 403 nm, which is broader and stronger than those of pure g-C3N4, CeO2 and kaolin, whereas the optical absorption edge is extended to around 430 nm. However, a low light absorption ability within the range of 445 nm was observed for the kaolin due to the light scattering effect. The band gaps of CeO2 and g-C3N4 were calculated based on Equation (1).
αhν = A(hν − Eg)n/2
where α, h, ν, A and Eg are the optical absorption coefficient, Planck constant, photon frequency, a constant and band gap, respectively. “n” denotes the type of electronic transitions, i.e., n = 1 or 4 shows a direct-allowed or indirect-allowed transition, respectively. Since g-C3N4 and CeO2 were indirect semiconductors, Eg was estimated from the plot of (αhν)1/2. Hence, band gaps of 2.73, 2.75 and 2.92 eV were calculated for kaolin/CeO2/g-C3N4 composite, g-C3N4 and CeO2, respectively. Subsequently, the band directly responsible for the interface migration of photoinduced charge carriers was estimated by the Mulliken electronegativity using Equations (2) and (3).
ECB = χp − Ee − 0.5Eg
EVB = ECB + Eg
where ECB and EVB are the edge potentials of conduction and valence bands, respectively, χp is the electronegativity of semiconductor, Ee is the energy of free electrons on the hydrogen scale (~4.5 eV), and Eg is the band gap energy of semiconductor. The valence band potentials (CB) of g-C3N4 and CeO2 are 1.82, and 2.04 eV, respectively. According to Equation (2), the conduction valence bands (VB) of g-C3N4 and CeO2 were estimated at −0.91, and −0.71 eV, respectively. According to Equation (3).
The specific surface area and pore volume of the as-prepared samples were evaluated from the N2 adsorption/desorption isotherms. As shown in Figure 5, the physisorption isotherms of all samples belong to type IV, which indicated their mesoporous structure. The values of the surface area, pore volume and pore diameter are listed in Table 1. The specific surface area of the kaolin/CeO2/g-C3N4 composite was 77.608 m2g−1, which was higher than that of kaolin (12.628 m2g−1), CeO2 (9.770 m2g−1) and g-C3N4 (29.936 m2g−1). The pore volumes of the kaolin/CeO2/g-C3N4 composite, kaolin, CeO2 and g-C3N4 were 0.129, 0.051, 0.033 and 0.079, respectively. The large surface area and pore volume of the kaolin/CeO2/g-C3N4 composite could be attributed to the uniform dispersion of CeO2 particles and the unique architecture of the composite, which could provide more adsorption and active sites and thus, an effective increase in photocatalytic activity.
3.2. Photocatalytic Activity
The photocatalytic activity of the samples was evaluated in the degradation of ciprofloxacin (CIP) under visible light irradiation. CIP, a typical antibiotic that is colorless in aqueous solution, can be effectively removed by the effect of photosensitization during visible-light-driven photodegradation process. As shown in Figure 6a, the mixture was kept in the dark for 60 min to achieve adsorption-desorption equilibrium between the antibiotic and photocatalyst. The removal efficiency of CIP was approx. 24% after 60 min in the presence of kaolin/CeO2/g-C3N4. After irradiation, CIP was degraded by kaolin/CeO2/g-C3N4. In the case of all samples, the kaolin/CeO2/g-C3N4 composite showed superior photocatalytic activity and 90% degradation efficiency of CIP was achieved after 150 min, while pure CeO2 and g-C3N4 degraded by approx. 42% and 51%, respectively. The enhanced photocatalytic performance was explained by the formation of heterojunctions between different materials and the abundant adsorption and active sites on the surface of layered kaolin, improved visible-light absorption and separation efficiency of photo-induced, electron-hole charges. As shown in Figure 6b, the photocatalytic degradation followed the first-order kinetics. The kinetics equation expressed by ln (C0/C) = kt, where C0/C is the normalized concentration of CIP, it is the reaction time, and k is the reaction rate constant (min−1), shows a linear relationship between ln (C0/C) and time. The results indicated that the rate constant of the reaction over kaolin/CeO2/g-C3N4 composite was of 0.01022 min−1, which was about 2.36 and 2.85 folds higher than those for pure CeO2 and g-C3N4, respectively. Overall, the construction of a heterojunction structure decorated on the layered kaolinite with enhanced visible light absorption ability and effective separation of carriers through chemical bond connection, resulted in an enhanced photoactivity activity of g-C3N4. The stability and reusability experiments were also applied to prove the potential of the ternary composite for practical applications. Figure 6c depicts the time-dependent absorption spectra of CIP degradation over the as-synthesized composite. Changes in UV-vis spectra of CIP in liquid phase over kaolin, CeO2, g-C3N4, kaolin/CeO2, kaolin/g-C3N4 and CeO2/g-C3N4 composite vs irradiation time are shown in Figure S2. A dramatic decrease in the characteristic absorption band of CIP at 273 nm could be observed. As shown in Figure 6d, the kaolin/CeO2/g-C3N4 composite exhibited excellent catalytic performance after four reaction cycles, demonstrating its recyclability and structural stability. The possible mechanism of the photocatalytic degradation of CIP over g-C3N4/TiO2/bentonite nanocomposite was proposed, as illustrated in Figure 7 [50,51,52].
3.3. Photocatalytic Mechanism
The electrochemical impedance spectroscopy (EIS) and transient photocurrent responses were carried out in order to further elaborate the photogenerated charge separation and electron transfer performance. As shown in Figure 8a, the smallest arc radius in the EIS Nyquist plot was obtained for the kaolin/CeO2/g-C3N4 composite, indicating a lower interfacial charge-transfer resistance and more effective separation and transfer of photo-generated electron−hole pairs at the interfaces created in the composite. Furthermore, the intensity of photocurrent produced in the kaolin/CeO2/g-C3N4 composite was obviously greater than those of kaolin, CeO2 and g-C3N4 (Figure 8b). Therefore, the highest charge separation efficiency occurred in the g-C3N4/CeO2/kaolin composite.
The radical trapping experiments were conducted to analyze the mechanism of photodegradation process based on the generated radicals. Isopropanol (IPA), disodium ethylenediaminetetraacetate (EDTA-2Na) and 1,4-benzoquinone (BQ) were employed as scavengers of hydroxyl radicals (•OH), holes (h+) and superoxide radicals (•O2−), respectively. As shown in Figure 9a, a slight change in photocatalytic efficiency was observed when IPA was used, suggesting that •OH was not the main active species in the photocatalytic degradation. The photocatalytic efficiency was significantly decreased in the presence of BQ, indicating that •O2− intensively influenced the photocatalytic reaction. The photocatalytic activity was evidently reduced when EDTA-2Na was used, indicating that the h+ also played a key role in CIP degradation. Hence, h+ and •O2− were the two main active species in the photocatalytic degradation of CIP solution.
DMPO spin-trapping EPR spectra were used to observe the active radicals involved in CIP photo-degradation process. The signals of DMPO−•O2− were detected under visible-light irradiation (Figure 9b), confirming that •O2− radicals were produced in the photocatalytic reaction. As shown in Figure 9c, a negligible resonance signal of DMPO−•OH under darkness and visible light irradiation was observed, suggesting that no or a few •OH radicals participated in the photocatalytic reaction. Hence, the h+ and •O2− were the principal active species in degradation of CIP.
The experimental results allowed to propose the mechanism of interfacial charge separation and transfer process as well as the possible photocatalytic mechanism involved in the degradation of CIP over a ternary kaolin/CeO2/g-C3N4 heterojunction. Both mechanisms are depicted in Figure 10. Due to the large specific areas and negative-charged characteristic, kaolin promoted an increase in the number of available surface active sites and the separation of the photo-induced carriers [45]. Under visible-light irradiation, CeO2 and g-C3N4 were both excited, and the photogenerated electrons in conduction band (CB) of g-C3N4 were transferred to CB of CeO2, whereas the photogenerated holes in the valence band (VB) of CeO2 were transferred to that of g-C3N4. The photogenerated electrons in CB of CeO2 (ECB = −0.71 eV) could reduce O2 to •O2− (E0O2/•O2− = −0.33 eV vs. NHE) [53]. The accumulated h+ in VB of the g-C3N4 could not directly oxidize the adsorbed H2O to produce the •OH, because EVB of the g-C3N4 was more negative than E0•OH/H2O (+2.38 eV vs. NHE) [54] as shown in the Table 2. Hence, h+ could directly react with the organic pollutant, which was consistent with the results of the radical trapping experiment. In summary, it can be stated that the h+ and •O2− active species played a significant role in the degradation process.
4. Conclusions In the present study, a novel ternary kaolin/CeO2/g-C3N4 heterojunction was fabricated via a sol-gel method followed by mild hydrothermal treatment. The morphological analysis and other characterizations confirmed the formation of heterojunction, which displayed a higher surface area (77.608 m2g−1) and the enhanced visible-light absorption. The kaolin/CeO2/g-C3N4 composite exhibited superior photocatalytic activity in CIP degradation under visible light irradiation, and CIP was completely removed within 150 min. The enhanced photocatalytic activity could be attributed to the enhanced light harvesting capability and effective separation of photo-induced electrons and holes. This study provided new insights into the construction of highly efficient ternary photocatalysts under visible-light irradiation with real potential for the organic pollutant degradation.
Enlarge this image.Figure 1.(a) XRD patterns of kaolin, CeO2, g-C3N4, kaolin/CeO2, kaolin/ g-C3N4, CeO2/g-C3N4 and kaolin/CeO2/g-C3N4 composite, (b) the corresponding enlarged area marked with dashed lines in Figure 1a.
Enlarge this image.Figure 2.(a) XPS spectrum of kaolin/CeO2/g-C3N4 composite, (b) Ce 3d, (c) O 1s, (d) C 1s and (e) N 1s (f) The EPR signals of CeO2, kaolin/CeO2/g-C3N4, g-C3N4 and kaolin.
Enlarge this image.Figure 3. FESEM images of kaolin/CeO2/g-C3N4 composite (a); TEM (b) and HRTEM images (c,d) of kaolin/CeO2/g-C3N4 composite.
Enlarge this image.Figure 4. UV-Vis diffuse reflectance spectra (DRS) (a) and band gaps (b) of kaolin, CeO2, g-C3N4 and the kaolin/CeO2/g-C3N4 composite.
Enlarge this image.Figure 5. N2 adsorption desorption isotherms of (a) kaolin, (b) CeO2, (c) g-C3N4 and (d) the kaolin/CeO2/g-C3N4 composite.
Enlarge this image.Figure 6.(a) Photocatalytic degradation of ciprofloxacin (CIP) under visible light irradiation, (b) Linear transform Ln(C0/C) of the kinetic curves of CIP under visible light irradiation, (c) The changes in UV-vis spectra of CIP in liquid phase over the kaolin/CeO2/g-C3N4 composite vs irradiation time (d) Reusability of the kaolin/CeO2/ g-C3N4 composite.
Enlarge this image.Figure 7. The mechanism of the photocatalytic degradation of CIP over the kaolin/CeO2/g-C3N4 nanocomposite.
Enlarge this image.Figure 8. Transient photocurrent and Nyquist plots from electrochemical impedance spectroscopy (EIS) data for the composite and reference samples. (a) Nyquist plots for kaolin, CeO2, g-C3N4 and kaolin/CeO2/g-C3N4 composite, (b) transient photocurrent produced in kaolin, CeO2, g-C3N4 and kaolin/CeO2/g-C3N4 composite.
Enlarge this image.Figure 9.(a) Trapping experiments of active species during photodegradation of CIP in the presence of kaolin/CeO2/g-C3N4 under visible light irradiation; (b) DMPO-•OH and (c) DMPO-•O2- adducts on kaolin/CeO2/g-C3N4 under visible light irradiation.
Enlarge this image.Figure 10. Schematic representation of electron transfer on the surface of the kaolin/CeO2/g-C3N4 heterostructure.
| Sample Name | Slope | Pore Volume (cm3/g) | Pore Diameter (nm) | C Constant | Surface Area (m2/g) |
|---|---|---|---|---|---|
| CeO2 | 341.548 | 0.0331 | 8.9552 | 24.305 | 9.77 |
| kaolin | 268.517 | 0.0507 | 13.6668 | 37.946 | 12.628 |
| g-C3N4 | 115.108 | 0.0787 | 19.4854 | 94.908 | 29.936 |
| kaolin/CeO2/g-C3N4 | 44.621 | 0.1286 | 31.0499 | 178.012 | 77.608 |
| Samples | ECB for NHEa/eV | EVB for NHE a/eV | Eg/eV |
|---|---|---|---|
| g-C3N4 | −0.91 | 1.82 | 2.73 |
| CeO2 | −0.71 | 2.04 | 2.75 |
a NHE: normal hydrogen electrode.
Supplementary Materials
The following are available online at https://www.mdpi.com/1996-1944/13/17/3811/s1. Figure S1. (b-f) element mapping of C, N, O, Si, and Ce for kaolin/CeO2/g-C3N4 composite, the upper left corner (a) shows the corresponding images. (g) EDS spectrum; Figure S2. The changes in UV-vis spectra of CIP in liquid phase over kaolin, CeO2, g-C3N4, kaolin/CeO2, kaolin/g-C3N4 and CeO2/g-C3N4 composite vs irradiation time.
Author Contributions
Conceptualization, Z.H.; project administration and supervision; L.L.; formal analysis, project administration, writing-original draft, writing-review and editing; Z.L.; project administration; J.W.; data curation and methodology, H.L. All authors have read and agreed to the published version of the manuscript.
Funding
National Natural Science Foundation of China (NSFC 41972261).
Acknowledgments
This work is supported by the National Natural Science Foundation of China (NSFC 41972261).
Conflicts of Interest
The authors declare no conflict of interest.
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Zhiquan Huang1,2, Leicheng Li1,*, Zhiping Li1, Huan Li1 and Jiaqi Wu1
1College of Geosciences and Engineering, North China University of Water Resources and Electric Power, Zhengzhou 450046, Henan, China
2Luoyang Institute of Science and Technology, Luoyang 471023, Henan, China
*Author to whom correspondence should be addressed.
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