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Visible Light Up-conversion of Bio-Carbon Quantum-Dot-Decorated TiO2 for Naphthalene Removal

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15 April 2024

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17 April 2024

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Abstract
In this study, carbon-quantum-dot (CQD)-decorated TiO2 was prepared using an ultrasonic doping method and applied in the photocatalytic degradation of naphthalene under sunlight irradiation. The CQDs were synthesized from a typical macroalgae via diluted sulfuric acid pretreatment and hydrothermal synthesis using an optimal design, i.e., 3 wt% and 200 oC, respectively. The CQD/TiO2 composite remarkably enhanced the photocatalytic activity. The degradation of naphthalene under a visible light environment indicated that there is a synergistic mechanism between CQDs and TiO2, in which the generation of reactive oxygen species is significantly triggered; in addition, the N that originated from the macroalgae accelerated the photocatalytic efficiency. Kinetic analysis showed that the photo-catalytic behavior of the CQD/TiO2 composite followed a pseudo-first-order equation. Consequently, our combined experimental approach not only provides a facile pretreatment process for bio-CQDs synthesis, but also delivers a suitable TiO2 photocatalyst for up-conversion, along with critical insights into the development of harmful macroalgae resources.
Keywords: 
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1. Introduction

Polycyclic aromatic hydrocarbons (PAHs) have teratogenic, carcinogenic, and mutagenic effects that likely threaten human health via bio-communication or the amplification of the food chain [1]. Among the diverse remediation technologies that can be applied to aquatic PAHs, TiO2 photocatalysis has garnered attention in recent years due its good photochemical stability, high catalytic efficiency and strong capacity for oxidation [2,3]. However, due to its wide band gap and high photo-generated electron–hole pair recombination rate [4], unmodified TiO2 is often less active in the visible region and exhibits low carrier utilization; these factors greatly limit its widespread application.
Many research endeavors have been dedicated to developing modified TiO2 photo-catalyst systems in order to maximize the utilization of visible light [5]; in these, carbon doping technologies have been found to help overcome some of the intrinsic shortcomings of TiO2, such as its low absorption and utilization of light, and to easily recombine photo-generated electrons and photo-generated holes [6]. Compared to other technologies utilized for the doping of carbon materials, CQDs are particularly attractive in this field due to their capacity for electron transfer, good photo-luminescence, up-conversion fluorescence performance, and facile tunability [7,8]. However, the top-down method utilized for the preparation of CQDs still has certain limitations; for example, the carbon precursors are usually limited to materials with a large area of sp2 hybridization. In comparison, the bottom-up synthesis method employed for the preparation of CQDs has been widely used due to its simplicity and practicability [9,10]. It is worth noting that the development of simple, low-consumption and gentle synthetic methods for the preparation of fluorescent CQDs and the use of readily available, inexpensive and environmentally friendly natural resources as green carbon precursors has become an active research area. Biomass, especially renewable biomass materials, has been widely used as a precursor for the preparation of CQDs, showing good photo-luminescence properties, low toxicity and good bio-compatibility [11,12]. However, its practical application is hindered by its low yield, low fluorescence intensity, and controllability, which are affected by its complex biological composition. Therefore, the preparation of CQDs from biomass, especially waste biomass, has become a research hotpot in recent years. With this in mind, a fast-growing macro-algae, i.e., Sargassum Horneri (S.H.), whose burst is defined as golden tide [13] was used as a CQD precursor.
On the other hand, the synergistic effect of CQD/TiO2 has been proven to effectively inhibit the recombination of electrons and holes and improve the photo-catalytic efficiency [14]. In CQD/TiO2 composites, CQDs are bonded to TiO2 by Ti-O-C bonding, and some electrons migrate to TiO2; this results in Ti3+ defects in the TiO2 matrix and a positive charge on the surface of the CQDs. As a result, Ti3+ can promote the adsorption of O2- on the surface of the photo-catalyst. Meanwhile, the excited electrons of the composites can be transferred from the valence band (VB) of the CQDs to the conduction band (CB) of TiO2. Sequentially, the electrons of CB in TiO2 react with O2 to form·O2-, and the holes on the surface of the CQDs further oxidize H2O to form ·OH free radicals; these two free radicals play a role in the degradation of contaminants. In addition, some visible light can be collected and up-converted into photons with a higher energy via CQDs. As an important electron reservoir, CQDs can collect and store photo-generated electrons from the CB of TiO2, thereby hindering the recombination of electron–hole pairs and further promoting photo-catalytic activity. Regarding TiO2, its light response generally ranges within the ultraviolet light region and is excited with difficulty by light sources larger than 420 nm because of the wide band gap. Meanwhile, CQDs can effectively up-convert visible light that has a wavelength greater than 420 nm into ultraviolet and near-ultraviolet light with a range of 350–550 nm [15,16]. Under light irradiation, the photo-generated electrons trapped on CQDs can further reduce the absorbed O2 to reactive ·O2–, the generation of which may depend on the separation efficiency of the photo-generated carriers and the number of photo-generated electrons captured by the CQDs. In particular, due to their graphite-like electronic structure and functional groups, CQDs can promote the adsorption of organic compounds by the complex, improve the area of contact with the target contaminants, and further carry out the photo-degradation process. It is worth mentioning that the measurement of the transport band gap of the CQDs and TiO2 is also crucial, as the optical properties, the separation, and the migration of electrons in photo-catalysts are the key factors that determine the photo-catalytic activity [17,18,19].
The surface of biomass CQDs is rich in oxygen-containing functional groups [20,21,22]; they are therefore able to combine with semiconductors such as TiO2 to form potential photo-catalysts. In recent years, algae and their derived carbon materials have been found to act as co-catalysts when coupled with TiO2 [23,24,25]. However, CQD/TiO2 photo-catalysts prepared using biomass are also affected by their complex biological composition. A suitable pretreatment method would destroy the cellulose of the natural plant structure and increase the specific surface area and porosity of the raw materials; therefore, the economic and facile pretreatment of biomass for sequential composite synthesis is still crucial and challenging. In order to improve the yield of carbon quantum dots, dilute acid can be used in the pretreatment of biomass, showing the ability to perform cellulose hydrolysis under relatively wild reaction conditions [26,27]. Therefore, the steps of our reaction are defined as follows: pretreatment with dilute acid, the hydrothermal preparation of CQDs, and the synthesis of CQD/TiO2 via ultrasonic dipping. Furthermore, the potential of CQD/TiO2 as a photo-catalyst was investigated in the aquatic degradation of naphthalene under visible light. The aims of this study were to build a facile pretreatment process for bio-CQDs synthesis, to obtain a suitable method for the visible light up-conversion of a bio-CQD-decorated TiO2 catalyst, and to find a potential industrial application for macroalgae.

2. Materials and methods

2.1. Materials

S.H. was collected from Wenzhou coastal area and washed with deionized water to remove salts and impurities on the surface, before being dried in an electric blast oven for 24 h. The dried S.H. was then ground and sieved through an 80-mesh sieve. Reagents were acquired from commercial suppliers and used without any further processing or purification. Titanium dioxide (P25, Degussa, 99.5%) was procured from Sinopharm Chemical reagent Co., Ltd., and chromatographic pure naphthalene was purchased from Aladdin Reagent Company. Analytically pure acetic acid, sulfuric acid (H2SO4), hydrochloric acid (HCl), sodium hydroxide (NaOH) and dichloromethane were purchased from Lingfeng Chemical Reagent Co., Ltd (Shanghai, China).

2.2. Preparation of CQDs and CQD/TiO2

Dilute sulfuric acid was dissolved using 50 mL of de-ionized water in a 100 mL beaker, and the solution was transferred to a 100 mL stainless steel reactor; it was then placed in a drying oven at a predetermined temperature for 3 h. After the reaction, the CQD solution was cooled to room temperature. Then, centrifugation was performed 3 times at a speed of 10000 r·min−1 to remove the large particles; this was followed by neutralization and separation using a 0.22 μm polyethersulfone membrane. Sequentially, the carbon quantum dot (CQD) solution was obtained and designated as CQDs(L) (L means liquid) (Figure S-1 in Supplementary material). The CQD solution was freeze-dried to obtain a solid powder of CQD; this was as designated as CQDs(S) (S means solid).

2.3. Characterization of CQDs and CQD/TiO2

The morphology, size and crystal lattice of the materials were analyzed using transmission electron microscopy with a Field Emission Gun (TEM, Tecnai G2 F30, FEI). In detail, the parameters were as follows: the excitation voltage was 300 kV, the line resolution was 0.1 nm, the point resolution was 0.2 nm, and the information resolution was 0.14 nm. A Fourier transform infrared spectrometer (FT-IR, Nicolet IS50) was used in the range of 400-4000 cm-1 with a resolution of 4 cm-1 to characterize the surface function groups of the composites. UV-Vis absorption measurements were carried out via UV-Vis diffuse reflectance spectrophotometry (DRS) (CARY 300, Agilent), with scanning in the range of 200-800 nm. The obtained data were processed according to the Tauc plot method. The surface chemical composition and chemical status of the CQD/TiO2 were investigated using X-ray photoelectron spectroscopy (XPS, Kratos Axis-Ultra). In this paper, Al/Mg was used as the radiation source. The test conditions were as follows: the excitation source was Al Kɑ (1487 eV), the target voltage was 15 kV, the current was 3 mA, the vacuum degree was 10-7 Pa, and the binding energy was corrected with C1s and a reference of 284.6 eV.

2.4. Photo-catalytic activity measurements

The photo-catalytic activity of the CQD/TiO2 composites was evaluated using naphthalene. The photo-degradation experiments were performed by using a photochemical reactor (PhChem-III, Newbit Technology Co., Ltd., China) equipped with a Xenon arc lamp (500W, XE-JY500) to simulate sunlight irradiation. The catalysts were added to 10 mL of naphthalene solution (40 mg L-1) and stirred for 60 min under dark conditions to ensure that adsorption–desorption equilibrium was reached before photo-catalysis was performed. During the photo-catalysis process, the concentrations of naphthalene were determined using gas chromatography (GC-112A, Shanghai Yidian Analytical Instrument Co., Ltd., China) , and the relative removal rate ® of naphthalene was calculated based on triplicate experiments in an air-conditioned room to prevent heat effects. The detection conditions were as follows: the column used was the Agilent DB-5 capillary column (30 m × 0.32 mm × 0.25 μm); the detector used was a hydrogen flame ionization detector; the detector temperature was 280 °C; the inlet temperature was 250 °C; the column temperature was programmed to be maintained at 60 °C for 1 min, 4 °C·min1 to 130 °C for 5 min, and then 20 °C·min-1 to 280 °C; the carrier gas used was high-purity nitrogen, with a flow rate of 2.5 mL·min-1; the hydrogen flow rate was 40 mL·min-1; and the air flow rate was 400 mL·min-1. The gas chromatography results were presented using the internal standard–standard curve method.

3. Results and discussion

3.1. Effect of dilute sulfuric acid pretreatment on CQDs

The pretreatment with dilute acid was performed to hydrolyze and destroy the natural plant structure of the cellulose and simultaneously increase the specific surface area and porosity of S.H. [28], as well as the yield of CQDs. This method is more convenient compared to both the traditional method using concentrated acid, from the viewpoint of contamination, or the method using ultra-low dilute acid, from the viewpoint of energy demand; this is due to the high temperature and pressure that this method requires. Based on the results, an optimized design was chosen, i.e., 3.0% H2SO4 and a hydrothermal condition of 200 oC; with this, there was an almost 10-fold increase in the CQD yield , rising from 2.3% to 18.9% (Figure S-2, S-3 in Supplementary Materials). Regarding the synthesis of the CQD/TiO2 nano-composite, 0.40 g of TiO2 and 1-10 mL of the CQDs(L) (Liquid form, abbreviated as L), in which 1 mL of CQDs(L) corresponded to 0.012 g of CQDs(S), were dispersed into 30 mL of deionized water and processed using ultrasonic irradiation for 30 min. The suspension was dried at 60 °C for 24 h to achieve a CQD/TiO2 composite.

3.2. Characterization of CQDs and CQD/TiO2

The TEM analysis indicated that the CQDs presented an approximately spherical nano-morphological distribution with a nanometer size. The CQDs had a good in-plane lattice with a spacing of 0.283 nm (Figure 1a), which is close to the (101) plane of graphite. The CQD/TiO2 had a good crystal plane spacing that was similar to that of TiO2, and the diameter of the CQDs had no obvious effect on the morphology of TiO2. This indicates that there was a good binding structure between the CQDs and TiO2. Meanwhile, after embedding CQDs into TiO2, the lattice spacing of the CQD/TiO2 composite was determined to be 0.328 nm (Figure 1b).

3.2. UV-Vis Analysis of CQD/TiO2

In the ultraviolet wave band, the light absorption of CQD/TiO2 is less than that of TiO2, but in the visible light region, the light absorption of the CQD/TiO2 composite material is greatly enhanced compared to that of TiO2 (Figure 2). Because the CQDs exhibit a higher LUMO (Lowest Unoccupied Molecular Orbital)) energy level than the TiO2, the electrons excited by visible light can be easily transferred from the LUMO energy level to the CB of TiO2, and the absorption intensity of the CQDTiO2 is much higher than that of TiO2 in the visible region [29]. The threshold wavelengths (λg) of the absorption spectra of simple TiO2 are obviously lower than those of the CQD/TiO2 composite, which is due to the near-infrared absorption characteristics of CQDs [30] (Figure S-4 in Supplementary Material). The light absorption redshift and range broadening significantly indicated the promotion of the photocatalytic performance [31]. Further calculations also showed that the binding energy of the CQD/TiO2 (3.00eV) was lower than that of TiO2 (3.20 eV), which meant that more excited electrons transferred from the VB to the CB; this led to the promotion of the photo-absorption of the composite. That is to say, the up-conversion performance of CQDs and their tight combination with TiO2 can effectively promote the red-shift of the absorption wavelength and effectively inhibit the recombination of electrons and holes.

3.3. FTIR Analysis of CQD/TiO2

The FT-IR spectra of different materials are illustrated in Figure 3. In the FTIR spectra, the broad and strong absorption band peak at 3370 cm-1 is assigned to the -OH stretching vibration, and the absorption peaks at 2900 cm-1 and 1700 cm-1 are the stretching vibration peaks of C-H and C=O, respectively. The conjugate characteristic absorption peak produced by C=C appears near 1400 cm-1, and the absorption peak at 650-900 cm-1 may be the benzene ring hydrogen absorption peaks of in-plane, out-of-plane and benzene ring skeleton bending vibration. The FTIR analysis indicates that carbonaceous groups were introduced on the surface of TiO2, thus confirming the formation of the CQD/TiO2 composite. Meanwhile, the combination of CQDs enhances the absorption intensity of the Ti-O bond at 1100 cm-1, and this peak is the characteristic absorption peak of the Ti-O bond. In addition, the CQD/TiO2 shows a strong capacity for absorption when the wave number is lower than 1000 cm-1, which may be related to the increased distance between atoms or lattices, and the characteristic absorption peaks of Ti-O-C.

3.4. XPS analysis of CQD/TiO2

To explore the surface chemical composition and related valence state of the CQD/TiO2, the XPS full spectrum is given in Figure 4. Figure 4a shows that the composite contains the elements Ti, O, C, S, and N. The Ti 2p spectrum exhibited two peaks at 454.72 eV and 460.53 eV, which corresponded to Ti 2p3/2 and Ti 2p1/2, respectively; these are assigned to Ti4+ 2p peaks [32,33]. The binding energy of Ti 2p is shifted from the standard value of TiO2, indicating that there is a new binding structure in the CQD/TiO2 composite. The binding energy of Ti 2p3/2 is lower than the standard value of 458.20 eV, indicating that the existence of CQDs makes the electron binding energy smaller and increases the electron density of TiO2. Figure 4c shows the C 1s spectrum. The peaks of the C 1s spectrum at 284.32 eV, 285.76 eV, and 288.21 eV are attributed to the C-C/C=C, C-O and C=O bonds, respectively. Figure 4d shows that the absorption peaks of 529.35 eV, 530.72 eV and 532.40 eV in the O 1s spectrum are the characteristic peaks of the Ti-O/·O2, C=O and C-O groups, indicating the composition of the surface of the CQD/TiO2 composite material. The peak at 529.35 eV was attributed to the oxygen in the crystal lattice (Ti-O/O2), and the other two peaks at 530.72 eV and 532.40 eV were attributed to the C=O and C-O groups, indicating that a hybrid might have been formed in the CQD/TiO2 by a Ti-O-C bond. Figure 4e and Figure 4f show the spectral lines of N 1s and S 2p. The absorption peaks of the N 1s spectrum at 396.50 eV and 398.00 eV are Ti-N and Ti-N-O bonds, respectively. The binding energies of S 2p 3/2 and S 2p1/2 are located at 165.3 eV and 166.8 eV, respectively, mainly due to the S-C-S bond. N and S originated from the biomass, and the latter also was enhanced by the inclusion of the dilute sulfuric acid pretreatment. The doping of N and S also promoted the performance, thus indicating the advantages of biomass self-assembly [34]. In summary, the XPS analysis confirmed the presence of CQDs and their TiO2 counterparts in the structure of the composites.

3.5. Photocatalytic Performance of CQD/TiO2 on Naphthalene Removal

In order to certify the photo-catalytic intensification of CQDs and the dilute acid treatment, the degradation of naphthalene was performed using different materials, as shown in Figure 5. The initial environment parameters were as follows: the naphthalene concentration was 40 mg·L-1 and the volume was 500 mL; the CQD/TiO2 was synthesized using a mixture with a ratio of 10 mL of CQDs to 0.40 g of TiO2; and 0.03 g of solid material was used. It can be seen that the photo-catalytic effect of CQD/TiO2 is the best among all the materials, indicating that the doping of CQDs is beneficial to the photo-catalytic performance. The sulfuric acid pretreatment helps the CQDs to promote adsorption, thus leading to their tight combination with TiO2 and promoting the photo-catalytic performance of CQD/TiO2.
It is worth mentioning that adsorption continued to play an important role regardless of whether the dark or light condition was used; this is because the CQDs continued to mix with biomass carbon. In particular, with the increase in the carbon content, the adsorption of biomass carbon becomes crucial to the formation of the composite; meanwhile, the increase in the proportion of TiO2 used makes the photocatalytic effect more obvious [28]. It could be found that the number of CQDs in the CQD/TIO2 composite leads to variations in the removal efficiency; for example, an overdose of CQDs in TiO2 may cause particle aggregation and pore blocking, and thus reduce the photo-catalytic efficiency (Figure 6-a). This overdose effect was most obvious with the composite mass; the photo-catalytic efficiency of the naphthalene solution was the best, at 86.63%, with the mass of CQD/TiO2 achieving 0.03 g (Figure 6-b). Regarding the pH effect, the composite catalyst had a good catalytic effect on naphthalene around pH=6 (Figure 6-c), which was greatly affected by TiO2; this increased the acid–basic balance to pHzpc ~6.39 [35,36]). When the pH value of the reaction system is less than pHzpc, the increase in H+ in the solution will cause Ti-OH2+ generation; this is suitable for attracting photo-generated electrons and thereby effectively reducing the recombination rate of photo-generated electrons and holes. The best dose of CQD/TiO2 could a result of the balance between two aspects, i.e., the active sites involved in the reaction, and the capacity of the receiving photons.

3.6. Photocatalytic Mechanism Analysis of CQD/TiO2 on Naphthalene Removal.

In this work, the results of FT-IR, ultraviolet–visible spectroscopy and fluorescence spectroscopy showed that there were abundant functional groups on the surface of the CQD/TiO2, and that the absorption peaks at wavenumbers lower than 1000 cm-1 were the characteristic absorption peaks of Ti-O-C. The band gap of CQD/TiO2 was reduced compared with that of TiO2, and the absorption band shifted to visible light. Furthermore, the XPS results also indicated the variation in the surface elements of the composites, and the results showed that the electron density of the outer layer of Ti increased and the electron binding energy decreased. In addition, the Ti 2p line showed that CQDs and TiO2 were bonded through Ti-O-C bonds. The mechanism is illustrated in Figure 7, i.e., the photo-induced electron transfer and redox properties of CQDs improve the separation time of electron–hole pairs of TiO2, prevent the recombination of electron-holes. This provides more time for the contaminants to diffuse to the reactive site, which accelerates the photocatalytic efficiency.
CQDs can be used as an electron reservoir during photocatalysis, and the excited electrons of CQD/TiO2 can be transferred from the valence band (VB) of CQDs to the conduction band (CB) of TiO2, thereby hindering the recombination of electron–hole pairs and further promoting the photocatalytic activity. The generation of reactive oxygen species (ROS) can be triggered by low-power visible light irradiation [37], i.e., the electrons of CB in TiO2 react with O2 to form ·O2-. The photogenerated electrons trapped on CQDs can further capture the absorbed O2 to reactive ·O2, and the holes on the surface of CQDs oxidize H2O to form ·OH [38,39]. This provides more time for the contaminants to diffuse to the reactive site, which accelerates the photocatalytic efficiency. In addition, the N originating from the biomass makes TiO2 exhibit p-type conductive properties [40,41], which makes it easier for electrons to transfer to CQDs and improves the photocatalytic efficiency.
Regarding the degradation of naphthalene, the existence of ·O2-and ·OH enable the breaking or cleaving of the ions trapped on CQDs; this leads to the further capture of absorbed O2 and reactive ·O2 on the hobenzene ring structure. There are two types of hydrogen on the naphthalene structure, namely α-H and β-H (Figure 8). Compared with β-H, α-H has a higher electron density and activity, which means that this site is more easily connected with free radicals. The surface of naphthalene molecules is positively charged, and the electrostatic attraction between atoms can promote the negatively charged ·OH attacks on H at the α position, causing the C at the α position to form hydroxyl derivatives and generate naphthol (products B and C). ·O2- further oxidizes naphthol to form C=O double bonds, forming naphthoquinone (product D). Naphthoquinone is further attacked by ·OH, leading to the cleavage of C‒C bonds to form aldehyde compounds. Due to free radical attack at C1 and C4, the resulting aldehyde group is easily oxidized to a carboxyl group, leading to the formation of the product E. These intermediates are further oxidized into smaller molecules and are eventually fully mineralized.

3.7. Kinetic Model Analysis of Naphthalene Removal by CQD/TiO2

The pseudo-first-order kinetic model, the second-order kinetic model, and the double exponential kinetic model were used to fit the photo-catalysis of CQD/TiO2. The relevant parameters of the kinetic model are shown in Table 1, and the fitting plots can be found in Figure S-6 (Supplementary Material). The results indicated that the pseudo-first-order rate equation provides the best interpretation of the photo-catalysis of naphthalene when the CQD/TiO2 is used. Meanwhile, the double exponential model provides the best fit for the CQDs, indicating that both physical and chemical processes are involved in the degradation of naphthalene using CQDs, and that a change was experienced after combination with TiO2. Thus, naphthalene can diffuse thoroughly towards the reaction active site, which accelerates the photo-catalytic reaction.

4. Conclusions

CQDs were prepared using a N,S-containing marine biomass and a simple hydrothermal method, and CQD/TiO2 composites were synthesized using an ultrasonic method. This work indicated that macroalgae could act as a good precursor for CQDs, whose adsorption and combination performance can be enhanced by dilute sulfuric acid pretreatment; this further enhances the synthesis of CQD/TiO2 and its photo-catalytic capacity. The nano-structure of CQDs means that they compound well with TiO2, and thus the photocatalytic performance of TiO2 can be significantly promoted under this synergistic effect. Generally speaking, the up-conversion performance of CQDs and their tight combination with TiO2 can be demonstrated by the redshift of the threshold wavelength, a decrease in the binding energy and the further promotion of electron transfer, which enable a better degradation capacity to be achieved under visible light. During the degradation process, CQDs can be used as electron reserves in photocatalysis, thereby promoting the separation efficiency of electron–hole pairs, and further free radicals. They also possess the advantages engendered by biocarbon adsorption due to the intermolecular accumulation of π-π. Therefore, under simulated light irradiation, CQD/TiO2 exhibits an excellent photocatalytic performance, and the removal of naphthalene is significantly higher than that of simple TiO2. However, the photo-catalytic efficiency of the composite material seems sensitive to pH, especially during direct recycle tests; however, weak acid treatments can maintain its stability (Figure S-7 in Supplementary Material), which indicates that the more careful modification of acid should be performed in future work.
Supplementary Material: Supplementary data and analysis related to this article can be found online.
This work was supported by the Natural Science Foundation of Zhejiang province (LY20B060008).

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Figure 1. TEM image of CQDs and CQD/TiO2: (a) 5 nm; (b) 10 nm.
Figure 1. TEM image of CQDs and CQD/TiO2: (a) 5 nm; (b) 10 nm.
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Figure 2. UV-Vis DRS result of CQD/TiO2 composite.
Figure 2. UV-Vis DRS result of CQD/TiO2 composite.
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Figure 3. FT-IR spectra of different materials: (a) CQDs (b) TiO2 (c) CQD/TiO2.
Figure 3. FT-IR spectra of different materials: (a) CQDs (b) TiO2 (c) CQD/TiO2.
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Figure 4. XPS spectra of CQD/TiO2 composite materials: (a) full spectrum; (b) Ti 2p spectrum; (c) C 1s spectrum; (d) O 1s spectrum; (e) N 1s spectrum; (f) S 2p spectrum; (g) Ti 2p spectrum of TiO2; (h) O 1s spectrum of TiO2.
Figure 4. XPS spectra of CQD/TiO2 composite materials: (a) full spectrum; (b) Ti 2p spectrum; (c) C 1s spectrum; (d) O 1s spectrum; (e) N 1s spectrum; (f) S 2p spectrum; (g) Ti 2p spectrum of TiO2; (h) O 1s spectrum of TiO2.
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Figure 5. Effect of different materials on photocatalytic reaction of naphthalene (N. P.  means without pretreatment using dilute sulfuric acid).
Figure 5. Effect of different materials on photocatalytic reaction of naphthalene (N. P.  means without pretreatment using dilute sulfuric acid).
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Figure 6. Effect photocatalytic degradation of CQD/TiO2 on naphthalene.
Figure 6. Effect photocatalytic degradation of CQD/TiO2 on naphthalene.
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Figure 7. Synergy mechanism of CQD/TiO2.
Figure 7. Synergy mechanism of CQD/TiO2.
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Figure 8. Degradation of naphthalene with CQD/TiO2: (a) the chemical structure of naphthalene; (b) electrostatic potential (ESP) distribution of naphthalene; (c) degradation pathway map of naphthalene.
Figure 8. Degradation of naphthalene with CQD/TiO2: (a) the chemical structure of naphthalene; (b) electrostatic potential (ESP) distribution of naphthalene; (c) degradation pathway map of naphthalene.
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Table 1. Kinetics parameters for the removal of naphthalene.
Table 1. Kinetics parameters for the removal of naphthalene.
Kinetic model Parameters Samples
CQD/TiO2 CQD/TiO2
(dark)
CQDs
Pseudo-first order k1x102/
(min-1)
0.603 0.008 0.104
R2 0.8968 0.8608 0.4932
Pseudo-second order k2x104/
(L·mg-1·min-1)
5.642 0.447 0.552
R2 0.7764 0.8480 0.5179
Double exponential A1 -41.89 -29.56 -28.14
A2 -41.89 -29.56 -28.14
k3 0.0588 0.0214 0.1529
k4 0.0588 0.0214 0.1529
R2 -0.4477 0.2531 0.9150
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