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Micromachines 2019, 10(1), 66; https://doi.org/10.3390/mi10010066
Growth Process and CQDs-modified Bi4Ti3O12 Square Plates with Enhanced Photocatalytic Performance
State Key Laboratory of Advanced Processing and Recycling of Non-ferrous Metals, Lanzhou University of Technology, Lanzhou 730050, China
Joint Laboratory for Extreme Conditions Matter Properties, Southwest University of Science and Technology, Mianyang 621010, China
Author to whom correspondence should be addressed.
Received: 27 December 2018 / Accepted: 16 January 2019 / Published: 18 January 2019
Bi4Ti3O12 square plates were synthesized via a hydrothermal route, and their growth process was systematically investigated. Carbon quantum dots (CQDs) were prepared using glucose as the carbon source, which were then assembled on the surface of Bi4Ti3O12 square plates via a hydrothermal route with the aim of enhancing the photocatalytic performance. XRD (X-ray powder diffraction), SEM (scanning electron microscopy), TEM (transmission electron microscopy), UV-vis DRS (diffuse reflectance spectroscopy), XPS (X-ray photoelectron spectroscopy), FTIR (Fourier transform infrared spectroscopy), PL (photoluminescence) spectroscopy, EIS (electrochemical impedance spectroscopy) and photocurrent spectroscopy were used to systematically characterize the as-prepared samples. It is demonstrated that the decoration of CQDs on Bi4Ti3O12 plates leads to an increased visible light absorption, slightly increased bandgap, increased photocurrent density, decreased charge-transfer resistance, and decreased PL intensity. Simulated sunlight and visible light were separately used as a light source to evaluate the photocatalytic activity of the samples toward the degradation of RhB in aqueous solution. Under both simulated sunlight and visible light irradiation, [email protected]4Ti3O12 composites with an appropriate amount of CQDs exhibit obviously enhanced photocatalytic performance. However, the decoration of excessive CQDs gives rise to a decrease in the photocatalytic activity. The enhanced photocatalytic activity of CQDs-modified Bi4Ti3O12 can be attributed to the following reasons: (1) The electron transfer between Bi4Ti3O12 and CQDs promotes an efficient separation of photogenerated electron/hole pairs in Bi4Ti3O12; (2) the up-conversion photoluminescence emitted from CQDs could induce the generation of additional electron/hole pairs in Bi4Ti3O12; and (3) the photoexcited electrons in CQDs could participate in the photocatalytic reactions.
Keywords:Bi4Ti3O12 square plates; CQDs; [email protected]4Ti3O12 composites; photodegradation of RhB; photocatalytic mechanism
To date, water pollution particularly caused by organic dyes and pigments generated from chemical industries is getting increasingly serious and poses a great threat to aquatic life and human health. In the context of energy shortage, how to use solar energy as the power source to deal with water pollution has become an important subject. To achieve this aim, recently, semiconductor-based photocatalysis has aroused tremendous interest [1,2,3,4,5,6]. Titanium dioxide and titanium-based oxide semiconductors have been extensively studied as an important class of semiconductor photocatalysts. Nevertheless, these semiconductor photocatalysts generally have a wide bandgap (Eg) greater than 3.0 eV and are photocatalytically active only under ultraviolet (UV) irradiation. This limits the utilization rate of solar energy. Furthermore, the photoexcited electrons (e−) and holes (h+) in the semiconductors easily undergo rapid geminate recombination, and thus, only a small fraction of the photoexcited carriers are able to participate in the photocatalytic reactions. This implies that the photon utilization rate is very low. Widening the light absorption range and promoting the photoexcited electron/hole pair separation are two of the key points to achieve an excellent photocatalyst with the best use of solar energy. Therefore, many strategies have been developed to modify semiconductor photocatalysts [7,8,9,10,11,12,13,14,15,16].
Low-dimension nanomaterials like graphene, carbon quantum dots (CQDs) and SiC nanowires offer great potential applications for biological labeling, bioimaging, drug delivery, energy conversion, optoelectronic devices, wave absorption and sensors due to their attractive properties [17,18,19,20,21,22,23,24,25,26,27,28]. In particular, photoexcited CQDs are excellent electron donors and electron acceptors. The interesting photoinduced electron transfer property suggests that CQDs can be used to modify photocatalysts with the aim of promoting the separation of photogenerated electron/hole pairs. Moreover, the PL up-conversion effect allows CQDs to harvest long-wavelength light (visible/near-infrared (vis/NIR) light) and then emit short-wavelength light (UV light). The emitted UV light can stimulate the generation of electron/hole pairs in wide-bandgap semiconductors like titanium-based oxides. Assembly of CQDs on the surface of semiconductors has become an important strategy for the design of excellent semiconductor photocatalysts capable of making full use of solar energy. Several examples of CQDs-modified photocatalysts with enhanced photocatalytic performance include CQDs/Bi2WO6, α-Bi2O3/C-dots, CQDs/BiOBr, and CQDs/g-C3N4 [29,30,31,32].
As an important titanium-based oxide semiconductor, bismuth titanate (Bi4Ti3O12) has been extensively studied owing to its pronounced photocatalytic activity toward the degradation of organic pollutants and water splitting into hydrogen [33,34,35,36,37]. Bi4Ti3O12 is composed of perovskite-like (Bi2Ti3O10)2− blocks regularly interleaved with (Bi2O2)2+ units, forming a special layer structure along the  direction (b-axis) . A polarization electric field is formed perpendicular to the (010) facet. Under the action of the polarization electric field, photogenerated electrons and holes are easily separated and migrate along the  direction to reach the (010) facet . The anisotropic layered structure suggests that the photocatalytic activity of Bi4Ti3O12 highly depends on its morphology. In our previous work, we synthesized large-sized Bi4Ti3O12 nanosheets with a highly exposed (010) facet via a hydrothermal route and found that their photocatalytic activity was much higher than that of Bi4Ti3O12 nanoparticles . On the other hand, Bi4Ti3O12 was frequently integrated with other semiconductors or decorated with noble metals to achieve excellent composite photocatalysts [40,41,42,43,44,45,46,47,48]. Very recently, Wang et al. reported on bamboo prepared CQDs for enhancing Bi4Ti3O12 photocatalytic activity . Their work demonstrated that CQDs were a good modifier to enhance the photocatalytic activity of Bi4Ti3O12, although only 65% of ciprofloxacin was observed to be degraded at 90 min of photocatalysis. Further increasing the photocatalytic performance and elucidating the enhanced photocatalytic mechanism of CQDs-modified Bi4Ti3O12 is still necessary. Here we report on an alternative method to assemble CQDs on Bi4Ti3O12 square plates. In the present study, glucose was used as the carbon source to produce CQDs. The preparation of CQDs and Bi4Ti3O12 square plates as well as the assembly of CQDs on Bi4Ti3O12 were carried out via a hydrothermal route. Moreover, the growth process of Bi4Ti3O12 square plates was systematically investigated. The characteristics, photocatalytic performance and photocatalytic mechanism of the as-prepared CQDs/Bi4Ti3O12 composites were systematically investigated and discussed.
2. Materials and Methods
2.1. Synthesis of Bi4Ti3O12 Square Plates
A hydrothermal route was used to synthesize Bi4Ti3O12 square plates. In a typical synthesis, 0.004 mol (1.9402 g) of Bi(NO3)3·5H2O was dissolved in 20 mL of 10% v/v dilute nitric acid solution (solution A), 0.003 mol (0.5691 g) of TiCl4 was dissolved in 20 mL of deionized water (solution B), and 0.2 mol (8 g) of NaOH was dissolved in 40 mL of deionized water (solution C). The solutions B and C were successively dropped in the solution A slowly with the aid of mild magnetic stirring. The resultant mixture was loaded and sealed into a 100 mL Teflon-lined stainless steel autoclave and subjected to heat treatment at 200 °C. To investigate the growth process of Bi4Ti3O12 square plates, different heat treatment temperatures (3, 6, 12, 24 and 36 h) were carried out. After the autoclave was naturally cooled to room temperature, the produced precipitate was collected by centrifugation, washed several times with deionized water and absolute ethanol, and dried at 60 °C for 12 h.
2.2. Assembly of CQDs on the Surface of Bi4Ti3O12 Square Plates
Bi4Ti3O12 square plates synthesized at 200 °C for 24 h via the above hydrothermal route were used to be decorated with CQDs in two steps. The first step was to prepare CQDs suspension using glucose as the carbon source. One gram of glucose was added to 80 mL deionized water, followed by ultrasonic treatment for 30 min and magnetic stirring for another 30 min. The glucose solution was then loaded into a Teflon-lined stainless steel autoclave (100 mL) and subjected to heat treatment at 180 °C for 4 h. After the autoclave was naturally cooled to room temperature, the solution was filtered through a millipore filter paper two times. The obtained reddish-brown solution was CQDs suspension. The second step was to assemble CQDs on the surface of Bi4Ti3O12 square plates. In a typical assembly process, 0.1 g of Bi4Ti3O12 plates was added into 70 mL of deionized water and ultrasonicated for 30 min. Ten milliliters of the CQDs suspension was added drop by drop into the Bi4Ti3O12 suspension and magnetically stirred for 1 h. The resultant mixture was loaded into a 100 mL Teflon-lined stainless steel autoclave and subjected to heat treatment at 130 °C for 4 h. After cooling to room temperature naturally, the precipitate was collected by centrifugation and dried at 60 °C for 12 h. The final product was obtained as the [email protected]4Ti3O12 composite. According to this procedure, several composite samples with different CQDs contents were prepared by adding different volumes of CQDs solution (5, 10, 15, and 20 mL) into the precursor Bi4Ti3O12 suspension, and the corresponding samples were designated as [email protected]4Ti3O12, [email protected]4Ti3O12, [email protected]4Ti3O12, and [email protected]4Ti3O12.
2.3. Sample Characterization
The crystal structure of the samples was identified by x-ray powder diffraction (XRD) with Cu Kα radiation (λ = 0.15406 nm) on a D8 Advance x-ray diffractometer (Bruker AXS, Karlsruhe, Germany). Scanning electron microscopy (SEM) and transmission electron microscopy (TEM) were used to investigate the morphology and microstructure of the samples. The SEM and TEM investigation was performed on a JSM-6701F scanning electron microscope (JEOL Ltd., Tokyo, Japan) and a JEM-1200EX transmission electron microscope (JEOL Ltd., Tokyo, Japan). Energy-dispersive x-ray spectroscopy (EDS) attached to TEM was used to analyze the chemical composition and elemental distribution of the samples. The optical absorption and bandgap energy of the samples were characterized by UV-vis diffuse reflectance spectroscopy (DRS) on a TU-1901 double beam UV-vis spectrophotometer (Beijing Purkinje General Instrument Co. Ltd., Beijing, China). X-ray photoelectron spectroscopy (XPS) measurement was carried out on a PHI-5702 multi-functional x-ray photoelectron spectrometer (Physical Electronics, hanhassen, MN, USA) to reveal the composition and chemical states of elements in the samples. Fourier transform infrared spectroscopy (FTIR) analysis was performed on a Spectrum Two FTIR spectrophotometer (PerkinElmer, Waltham, MA, USA) in the range of 500–4000 cm−1 using KBr powder. A RF-6000 fluorescence spectrophotometer (Shimadzu, Kyoto, Japan) was used to measure the photoluminescence (PL) spectra of the samples with an excitation wavelength of 320 nm.
2.4. Photocatalytic Testing
Simulated sunlight emitted by a 200 W xenon lamp (300 < λ < 2500 nm) and visible light generated by a 200 W halogen-tungsten lamp (λ > 400 nm) were separately used as the light source to evaluate the photocatalytic activity of the samples toward the degradation of rhodamine B (RhB) in aqueous solution. Such as in a typical photocatalytic experiment, 0.2 g of the photocatalyst was loaded into 100 mL of 5 mg·L−1 RhB aqueous solution. The mixture was put into the photoreactor and magnetically stirred in the dark for 30 min to determine the adsorption of RhB onto the photocatalyst surface. During the photocatalytic process, a circulating water cooling system was used to cool the photoreactor in order to maintain the reaction solution at room temperature (~21 °C). The residual concentration of RhB was monitored every 30 min. To achieve this, 2.5 mL of the reaction solution was sampled from the photoreactor and centrifugated to remove the photocatalyst. The residual concentration of RhB was determined by measuring the absorbance of the reaction solution on a UV–vis spectrophotometer at λ = 554 nm. The degradation percentage of RhB is defined as follows: D% = (1 − Ct/C0) × 100%, where C0 and Ct represent the initial and residual RhB concentrations after photocatalysis for t min.
2.5 Electrochemical Measurement
A three-electrode cell configuration was used for the transient photocurrent response and electrochemical impedance spectroscopy (EIS) measurements of the samples on a CST 350 electrochemical workstation (Wuhan Corrtest Instruments Co. Ltd., Wuhan, China) [50,51]. A platinum foil electrode and a standard calomel electrode (SCE) were used as the counter electrode and reference electrode, respectively. The working electrode was prepared following the procedure described in the literature . Stoichiometric amounts of the photocatalyst (15 mg), acetylene black (0.75 mg) and polyvinylidene fluoride (PVDF, 0.75 mg) were uniformly mixed into 1 mL 1-methyl-2-pyrrolidione (NMP) that acted as the dispersant. The paste mixture was homogeneously coated onto fluorine-doped tin oxide (FTO) glass substrate (effective area: 1 × 1 cm2). After drying at 60 °C for 5 h, the final working electrode was obtained. The electrolyte used in this study is a Na2SO4 aqueous solution with a concentration of 0.1 mol·L−1. Simulated sunlight emitted from a 200 W xenon lamp was used as the light source. The transient photocurrent response measurement was performed at a bias potential of 0.2 V. The EIS measurement was performed by imposing a small sinusoidal voltage of 5 mV amplitude over the frequency range from 100 kHz to 0.01 Hz. To investigate the flat band potential of Bi4Ti3O12, the EIS was measured at different applied potentials in the dark.
3. Results and Discussion
3.1. Growth Process of Bi4Ti3O12 Square Plates
Figure 1 shows the XRD patterns of Bi4Ti3O12 samples prepared at 200 °C with different reaction times (t = 3, 6, 12, 24, and 36 h). It is seen that the sample obtained at t = 3 h consists of a mixture of phases including Bi4Ti3O12 (PDF#35-0795), Bi2O3 (PDF#27-0050) and anatase TiO2 (PDF#21-1272). Moreover, a broad peak at around 2θ = 10° is observed on the XRD pattern, which arises from the amorphous Bi(OH)3 and Ti(OH)4 precipitates hydrolyzed from Bi(NO3)3 and TiCl4. When the reaction time is increased up to 6 h, the diffraction peaks related to Bi2O3, TiO2 and amorphous substances disappear. All the diffraction peaks can be indexed according to the standard diffraction pattern of PDF#35-0795, implying the formation of a single Bi4Ti3O12 orthorhombic phase. With prolonging the reaction time, the prepared samples maintain a pure Bi4Ti3O12 orthorhombic phase without the appearance of other impurities.
Figure 2 shows the SEM images of Bi4Ti3O12 samples prepared at different reaction times (t = 3, 6, 12, 24, and 36 h). As shown in Figure 2a, the product obtained at 3 h reaction time is composed of nanorods, spherical nanoparticles and amorphous aggregates, which are characterized as Bi4Ti3O12, Bi2O3, TiO2, and Bi(OH)3/Ti(OH)4 precipitates. At 6 h reaction time (Figure 2b), the Bi2O3/TiO2 spherical nanoparticles and Bi(OH)3/Ti(OH)4 precipitates are crystallized into Bi4Ti3O12 nanorods. With further increasing the reaction time up to 12 h (Figure 2c), the formed Bi4Ti3O12 nanorods gradually grow into brick-like nanoparticles. When the reaction time is increased up to 24 h (Figure 2d,e), it brings about the synthesis of Bi4Ti3O12 square plates with an average lateral size of ~1 μm and thickness of ~200 nm. However, too long a reaction time leads to partial dissolution of the square plates into small-sized brick-like nanoparticles, as shown in Figure 2f.
Based on the XRD and SEM results, the formation process of Bi4Ti3O12 square plates is schematically illustrated in Figure 3. The ‘‘dissolution–crystallization’’ mechanism can be used to describe the hydrothermal formation of Bi4Ti3O12 square plates . In the precursor solution, Bi(NO3)3·and TiCl4 were hydrolyzed into Bi(OH)3 and Ti(OH)4 hydroxides with the aid of NaOH. At high temperature and pressure environments, the Bi(OH)3 and Ti(OH)4 precipitates are to dissolve and form ion groups under the action of NaOH that serves as the mineralizer. In the locally formed supersaturated fluid region, Bi4Ti3O12 nanorods are crystallized by nucleation, precipitation, dehydration, and growth. Simultaneously, Bi2O3 and TiO2 could also be formed in this process. With the hydrothermal reaction going on, Bi2O3 and TiO2 will dissolve again to form ion groups under the attack of NaOH, which will then subsequently crystallize into Bi4Ti3O12 nanorods. The formation of Bi4Ti3O12 crystals can be simply described by Equations (1) and (2). With increasing the reaction time, Bi4Ti3O12 nanorods gradually grow into brick-like nanoparticles and then into square plates. The formation of Bi4Ti3O12 square plates can be explained as a result of the reduction of the overall surface energy. It is noted that the growth process of Bi4Ti3O12 square plates is simultaneously accompanied by their dissolution process. After a relatively long reaction time, the dissolution process could predominate over the growth process, and as a result, Bi4Ti3O12 square plates are etched into small-sized brick-like nanoparticles.
4Bi(OH)3 + 3Ti(OH)4 → Bi4Ti3O12 + 12H2O
2Bi2O3 + 3TiO2 → Bi4Ti3O12
3.2. CQDs-modified Bi4Ti3O12 Square Plates
The photocatalytic activity of the as-prepared [email protected]4Ti3O12 composites was evaluated by the degradation of RhB in aqueous solution separately under the irradiation of simulated sunlight (300 < λ < 2500 nm) and visible light (λ > 400 nm). Before the photocatalytic degradation experiment, the adsorption of RhB onto bare Bi4Ti3O12 and [email protected]4Ti3O12 composites was measured in the dark at 30 min of contact time and is obtained as 3.5‒15.3%. It is observed that the RhB adsorption gradually increases with increasing the CQDs content, which is ascribed to the enhanced dye adsorption of CQDs. Generally, an appropriate increase in the dye adsorption is conducive to photocatalysis. The time-dependent photocatalytic degradation of RhB under simulated sunlight irradiation is shown in Figure 4a. The degradation percentage of RhB after 120 min of photocatalysis is given in Table 1. It is seen that the decoration of an appropriate amount of CQDs on Bi4Ti3O12 leads to a significantly enhanced photocatalytic activity. The highest photocatalytic performance is observed for the [email protected]4Ti3O12 composite prepared by adding 10 mL CQDs solution, and the degradation percentage of RhB reaches 94.3%. However, decoration of excessive CQDs on Bi4Ti3O12 could reduce the light absorption of Bi4Ti3O12, and thus, give rise to a decrease in the photocatalytic activity. To further compare the photocatalytic activity between the samples, the degradation kinetics of RhB were investigated. As shown in Figure 4b, the plots of Ln(Ct/C0) vs irradiation time t can be well modeled using the pseudo-first-order kinetic equation: Ln(Ct/C0) = −kappt, where kapp is the apparent first-order reaction rate constant . The obtained value of kapp from the slope of the regression lines is given in Table 1. It is seen that the optimal composite [email protected]4Ti3O12 manifests a photocatalytic activity ca. 1.8 times higher than that of bare Bi4Ti3O12. Figure 4c shows the visible-light photocatalytic degradation of RhB over bare Bi4Ti3O12 and [email protected]4Ti3O12 composites, and Figure 4d presents the plots of Ln(Ct/C0) vs irradiation time t. The obtained degradation percentage after photocatalytic reaction for 120 min and reaction rate constant kapp are summarized in Table 1. Photocatalyzed by bare Bi4Ti3O12, only 15.7% of the dye is observed to be degraded, which is mainly ascribed to the dye adsorption and dye-photosensitized degradation. This indicates that bare Bi4Ti3O12 exhibits poor photocatalytic activity under visible light irradiation. When compared with bare Bi4Ti3O12, the [email protected]4Ti3O12 composites manifest a greatly enhanced visible-light photocatalytic activity. In particular, the [email protected]4Ti3O12 composite photocatalyzes 42.4% removal of the dye and displays a photocatalytic activity ca. 3.2 times as large as that of bare Bi4Ti3O12 according to the reaction rate constants.
Further investigation was specially carried out on the [email protected]4Ti3O12 composite prepared with 10 mL CQDs solution with the aim of revealing its microstructure and enhanced photocatalytic mechanism. Figure 5a–c shows the TEM images of [email protected]4Ti3O12. It is seen that Bi4Ti3O12 has a geometrical morphology of square plates. Occasionally, the square plates are assembled into a T-shape structure, as shown in Figure 5b. Figure 5d shows the selected area electron diffraction (SAED) pattern obtained from the Bi4Ti3O12 square plate of Figure 5c. The diffraction spots are regularly and periodically arranged, which can be indexed to the  zone axis of Bi4Ti3O12 orthorhombic structure. The a-axis and b-axis are parallel to the lateral side of the square plate. The highly exposed plane of the square plate is identified to be the (010) facet. This crystallographic orientation of the Bi4Ti3O12 square plate is further confirmed by the high resolution TEM (HRTEM) image, as shown in Figure 5e. The lattice fringes with d-spacing of 0.384 nm are observed to be parallel or perpendicular to the diagonal direction of the square plate and match well with the (202) crystal plane of Bi4Ti3O12 orthorhombic phase. Although the TEM/HRTEM images and SAED pattern cannot show the presence of CQDs on Bi4Ti3O12 plates, other methods can be used to determine the formation of [email protected]4Ti3O12 composites. Figure 5f shows the dark-field scanning TEM (DF-STEM) image of the [email protected]4Ti3O12 composite, and Figure 5g–j presents the corresponding energy-dispersive x-ray elemental mapping images of the region marked by the orange rectangle in Figure 5f. Besides the elements of Bi, Ti and O which constitute Bi4Ti3O12 square plates, C element is also observed to be uniformly distributed throughout the plates. The elemental mapping images confirm the uniform assembly of CQDs on the surface of Bi4Ti3O12 plates. The chemical composition of [email protected]4Ti3O12 was further investigated by EDS spectrum, as shown in Figure 5k. It is obvious that the [email protected]4Ti3O12 sample is composed of Bi, Ti, O, and C elements. The observed Cu signal on the EDS spectrum could arise from the microgrid used for supporting the sample in the TEM experiment . The Bi/Ti atomic ratio obtained from the EDS spectrum is very close to that in the Bi4Ti3O12 phase. However, the EDS spectrum shows a lower O content with respect to oxygen in Bi4Ti3O12, which could be ascribed to non-sensitivity of EDS to light elements like O .
Figure 6 shows the XRD patterns of Bi4Ti3O12 and [email protected]4Ti3O12. It is seen that the diffraction peaks of [email protected]4Ti3O12 are very similar to those of bare Bi4Ti3O12, implying that Bi4Ti3O12 undergoes no structural change when assembled with CQDs. No obvious diffraction signals assignable to CQDs are detected in the XRD pattern. The possible reason may be that CQDs have extremely weak x-ray diffraction due to the lack of long-range-ordered structure, and moreover, CQDs account for only a small fraction of the total mass of the [email protected]4Ti3O12 composite.
Figure 7a,b shows the UV-vis DRS spectra of Bi4Ti3O12 and [email protected]4Ti3O12. A significantly enhanced light absorption in the wavelength range of 400‒850 nm is observed for the [email protected]4Ti3O12 composite when compared with bare Bi4Ti3O12. The digital images of the samples separately inserted in Figure 7a,b demonstrate that bare Bi4Ti3O12 is cream white, whereas [email protected]4Ti3O12 manifests a gray color. The deepening of the apparent color for [email protected]4Ti3O12 further confirms its enhanced visible-light absorption. This implies that the composite can make more efficient utilization of sunlight during photocatalysis. The first derivative curves of the UV-vis DRS spectra are used to determine the absorption edge of the samples . As seen from Figure 7a,b, Bi4Ti3O12 and [email protected]4Ti3O12 exhibit an absorption edge of 372.2 and 364.4 nm, respectively. Based on the absorption edge, the bandgap energy (Eg) can be derived from the relationship Eg = 1240/λabs (λabs represents the absorption edge wavelength), and is obtained as 3.33 eV for bare Bi4Ti3O12 and 3.40 eV for [email protected]4Ti3O12. The slight increase in the Eg of the composite could be ascribed to the interaction between Bi4Ti3O12 plates and CQDs.
XPS analysis was carried out to reveal the composition and element chemical states of the [email protected]4Ti3O12 composite. Figure 8a shows the XPS survey scan spectrum, revealing the existence of Bi, Ti, O, and C elements in the composite. Figure 8b–e illustrates the high resolution XPS spectra of Bi 4f, Ti 2p, O 1s, and C 1s, respectively. As seen from Figure 8b, the Bi 4f XPS spectrum shows two sharp peaks at 158.9 and 164.2 eV, which are attributed to the Bi 4f7/2 and Bi 4f5/2 binding energies, respectively [33,56,57]. The Ti 2p XPS spectrum shown in Figure 8c can be deconvoluted into three peaks at 457.9, 463.5 and 465.9 eV, which correspond to the binding energies of Ti 2p3/2, Ti 2p1/2 and Bi 4d3/2 respectively [56,57]. The Bi 4f and Ti 2p binding energy peaks suggest that bismuth species exists in +3 oxidation state and titanium species exhibits +4 oxidation state. The existence of other oxidation states can be excluded since no additional binding energy peaks are detected on the Bi 4f and Ti 2p XPS spectra. On the O 1s XPS spectrum (Figure 8d), the binding energy at 529.7 eV is attributed to the crystal lattice oxygen of Bi4Ti3O12, whereas the binding energy at 531.5 eV could arise from chemisorbed oxygen species [58,59]. The C 1s XPS spectrum (Figure 8e) presents two peaks at 284.8 and 287.7 eV. The peak at 284.8 eV arises from the C–C sp2-hybridized carbon of CQDs and adventitious carbon that is used to calibrate the binding energy scale [59,60]. The peak at 287.7 eV is attributed to the presence of C–O–C or C=O .
The functional groups of Bi4Ti3O12 and [email protected]4Ti3O12 were analyzed by FTIR spectra, as shown in Figure 9a. The broad bands detected at 3430 and 1637 cm−1 correspond to the stretching and bending vibrations of water molecules absorbed on the surface of the samples, respectively . The peaks observed at 1102 and 1395 cm−1 account for the C–OH stretching and O–H in-plane deformation vibrations of alcohols left on the samples during their washing process. The broad absorption band at around 3146 cm−1 is assigned to the N–H stretching vibration of the NH3+ group . The strong peak at 477 cm−1 and weak peak at 586 cm−1 are characterized as the Ti–O stretching vibration. The characteristic stretching vibration of Bi–O is observed at 819 cm−1 [63,64]. This implies the formation of the Bi4Ti3O12 orthorhombic phase and its crystal structure undergoes no destruction when decorated with CQDs. Additional peaks at 638, 1270, 1467, and 1620 cm−1 are detected for the [email protected]4Ti3O12 composite. The former two peaks (638 and 1270 cm−1) are ascribed to the C–H deformation vibration and the latter two peaks (1467 and 1620 cm−1) can be attributed to the C–C stretching vibration . These absorption peaks suggest that CQDs are assembled on the surface of Bi4Ti3O12 plates.
To reveal the separation and transfer behavior of photogenerated electrons and holes, PL, photocurrent response and EIS analyses were carried out. Figure 9b shows the PL spectra of Bi4Ti3O12 and [email protected]4Ti3O12 measured at an excitation wavelength of 320 nm. Both samples clearly display the PL emission peaks at 448, 466, 480, and 491 nm, which arise due to the recombination of photogenerated electron/hole pairs. When compared with bare Bi4Ti3O12, the [email protected]4Ti3O12 composite exhibits the PL emission peaks with relatively lower intensity, implying a decreased electron/hole recombination. The efficient separation of electron/hole pairs occurring in the composite can be explained as a result of the electron transfer from the conduction band (CB) of Bi4Ti3O12 to CQDs.
Figure 9c shows the transient photocurrent response curves of Bi4Ti3O12 and [email protected]4Ti3O12 measured under intermittent irradiation of simulated sunlight with 10 min irradiation followed by 10 min intervals. When the simulated sunlight is turned off, a photocurrent density of ca. 0.10–0.16 and 0.34–0.37 μA·cm−2 is observed for bare Bi4Ti3O12 and [email protected]4Ti3O12, respectively. The photocurrent density for both samples immediately drops almost to zero when the light is turned off. This effect appears to be very reproducible upon alternately turning on and off the light. The transient photocurrent measurement clearly demonstrates that the [email protected]4Ti3O12 composite exhibits a more efficient separation of photogenerated electron/hole pairs than bare Bi4Ti3O12. This result is further confirmed by the Nyquist plots of the EIS spectra, as shown in Figure 9d. It is clearly seen that the Nyquist plots of both samples display a semicircle (high-frequency region) followed by a straight line (low-frequency region). However, a smaller semicircle diameter is observed for the composite. It is well established that the semicircle diameter of the Nyquist plots is correlated with the charge-transfer resistance at the electrode/electrolyte interface, and a smaller diameter suggests a smaller charge-transfer resistance [66,67]. The EIS spectrum analysis elucidates an enhanced electron/hole pair separation and interface charge transfer under irradiation of simulated sunlight for the [email protected]4Ti3O12 composite.
Based on the aforementioned experimental results and analyses, a possible photocatalytic mechanism of [email protected]4Ti3O12 toward the dye degradation is proposed, as schematically illustrated in Figure 10. Under simulated sunlight irradiation, electrons are excited from the valence band (VB) of Bi4Ti3O12 to its CB, thus creating electron/hole pairs. Simultaneously, the electronic excitation process also occurs in CQDs, i.e., electrons in the π orbital or σ orbital of CQDs are excited to a high-energy state such as the lowest unoccupied molecular orbital (LUMO) . The photoexcited CQDs are excellent electron donors and electron acceptors. As a result, the CB electrons in Bi4Ti3O12 will transfer to the π orbital or σ orbital of CQDs. Conversely, the photoexcited electrons in CQDs can be also transferred to the CB of Bi4Ti3O12. The interesting electron transfer process can efficiently suppress the recombination of photogenerated electron/hole pairs in Bi4Ti3O12. Consequently, more photogenerated carriers are able to participate in the photocatalytic reactions, thus leading to an increased photocatalytic performance of the [email protected]4Ti3O12 composites under simulated sunlight irradiation. It is noted that the Bi4Ti3O12 square plates have a bandgap of 3.33 eV, implying that bare Bi4Ti3O12 plates exhibit a poor photocatalytic activity under visible light irradiation. However, when CQDs are decorated on Bi4Ti3O12, the obtained [email protected]4Ti3O12 composites manifest an obviously enhanced visible-light photocatalytic activity toward the dye degradation, as shown in Figure 4c,d. This phenomenon can be attributed to the following reasons. Under visible light irradiation, the π electrons in CQDs could be excited to the LUMO. When the electrons fall back to the σ orbital, an up-conversion photoluminescence is emitted . The up-conversion photoluminescence could have photon energy larger than the bandgap energy of Bi4Ti3O12 and would induce the electron excitation from the VB to the CB of Bi4Ti3O12. The PL-induced electrons and holes are able to participate in the photocatalytic reactions. On the other hand, the photoexcited electrons in CQDs could also participate in the photocatalytic reactions. The two factors collectively result in the enhanced visible-light photocatalytic activity of the [email protected]4Ti3O12 composites.
Reactive species trapping experiments were carried out to reveal their role in the degradation of RhB over [email protected]4Ti3O12. In this study, ethanol, benzoquinone (BQ) and ammonium oxalate (AO) were used as the scavengers of hydroxyl (•OH), superoxide (•O2−) and photogenerated h+, respectively . Figure 11a shows the effect of ethanol (5 mL), BQ (0.1 mmol) and AO (0.1 mmol) on the degradation percentage of RhB at 120 min of photocatalysis. It is seen that the addition of ethanol to the reaction solution has almost no effect on the dye degradation, implying a minor or negligible role of •OH in the dye degradation. The addition of BQ leads to a slight suppression of the dye degradation. This suggests that the role of •O2− cannot be neglected, but it plays only a slight role in the photocatalytic reaction. With the addition of AO, however, the dye degradation is significantly suppressed and only 19.7% of RhB is observed to be degraded. This indicates that the photogenerated h+ is the dominant active species responsible for the dye degradation. To reveal the CB and VB potentials of Bi4Ti3O12 square plates, we carried out the Mott–Schottky measurement according to the method described in the literature [69,70,71], as shown in Figure 11b. By extrapolating the linear portion of the Mott–Schottky plot to the V axis, the flat band potential (VFB) is obtained as –0.75 V vs SCE. The SCE potential can be converted to the potential against a normal hydrogen electrode (NHE) using V(NHE) = V(SCE) + 0.059pH + 0.242 (here pH = 7) . The positive slope of the Mott–Schottky plot suggests that Bi4Ti3O12 exhibits an n-type semiconductivity. Assuming that the gap between the flat band potential and the CB edge is negligible for an n-type semiconductor, the CB potential of Bi4Ti3O12 square plates is therefore estimated as –0.10 V vs NHE. Their VB potential is obtained as +3.23 V vs NHE using VVB = VCB − Eg (Eg = 3.33 V). It is noted that the VB potential of Bi4Ti3O12 is more positive than the redox potentials of H2O/•OH (+2.38 V vs NHE) and OH−/•OH (+1.99 V vs NHE) . However, the reactive species trapping experiments demonstrate that •OH plays a negligible role in the dye degradation. To further confirm this, we also measured •OH radicals by PL spectroscopy using terephthalic acid as a probe of •OH, as described in the literature . Nevertheless, no •OH radicals are detected in the [email protected]4Ti3O12 photocatalytic system. The generation of minor •O2− radicals could be derived from the reaction of adsorbed O2 molecules with the photoexcited electrons in CQDs or photogenerated electrons at higher excited states of Bi4Ti3O12.
A hydrothermal route was used to synthesize Bi4Ti3O12 square plates with an average lateral size of ~1 μm and average thickness of ~200 nm. The growth process of the square plates was systematically investigated. CQDs derived from glucose were assembled on the surface of Bi4Ti3O12 square plates via a hydrothermal route. Compared to bare Bi4Ti3O12, the as-prepared [email protected]4Ti3O12 composites with an appropriate amount of CQDs manifest an increased photocatalytic performance for the RhB degradation under irradiation of simulated sunlight and visible light. The optimal [email protected]4Ti3O12 composite photocatalyzes 94.3% removal of the dye under simulated sunlight irradiation, demonstrating a photocatalytic activity ca. 1.8 times higher than that of bare Bi4Ti3O12. The enhanced photocatalytic performance of CQDs-modified Bi4Ti3O12 is mainly attributed to the efficient separation of photogenerated electron/hole pairs and increased visible light absorption. The efficient utilization of visible light during the photocatalysis is manifested in 2 aspects: (1) The visible-light photoexcited electrons in CQDs could participate in the photocatalytic reactions, and (2) additional electron/hole pairs in Bi4Ti3O12 could be generated by the up-conversion photoluminescence emitted from CQDs.
H.Y. conceived the idea of experiment; X.Z. and Z.M.C. performed the experiments; H.Y., X.Z., Z.M.C., X.X.W. and Z.Y. discussed the results; H.Y. wrote the manuscript; all authors read and approved the final manuscript.
This work was supported by the National Natural Science Foundation of China (Grant No. 51662027) and the HongLiu First-Class Disciplines Development Program of Lanzhou University of Technology.
Conflicts of Interest
The authors declare that they have no competing interests.
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Figure 1. XRD patterns of Bi4Ti3O12 samples prepared at 200 °C with different reaction times (t = 3, 6, 12, 24, and 36 h).
Figure 2. SEM images of Bi4Ti3O12 samples prepared at different reaction times (t = 3, 6, 12, 24, and 36 h).
Figure 3. Schematic illustration of the formation process of Bi4Ti3O12 square plates.
Figure 4. (a) Time-dependent photocatalytic degradation of RhB over Bi4Ti3O12 and [email protected]4Ti3O12 composites with different CQDs contents under simulated sunlight irradiation. (b) Degradation kinetic plots of RhB over the samples under simulated sunlight irradiation. (c) Time-dependent photocatalytic degradation of RhB over the samples under visible light irradiation. (d) Degradation kinetic plots of RhB over the samples under visible light irradiation.
Figure 5. (a‒c) TEM images of [email protected]4Ti3O12. (d) and (e) SAED pattern and HRTEM image obtained from the Bi4Ti3O12 square plate of (c), respectively. (f) DF-STEM image of [email protected]4Ti3O12. (g–j) The corresponding energy-dispersive x-ray elemental mapping images of the region marked by orange rectangle in (f). (k) EDS spectrum of [email protected]4Ti3O12.
Figure 6. XRD patterns of Bi4Ti3O12 and [email protected]4Ti3O12.
Figure 7. UV-vis DRS spectra, first derivative curves of the UV-vis DRS spectra and digital images of (a) Bi4Ti3O12 and (b) [email protected]4Ti3O12.
Figure 8. XPS spectra of [email protected]4Ti3O12. (a) Survey scan spectrum; (b)–(e) High resolution XPS spectra of Bi 4f, Ti 2p, O 1s, and C 1s, respectively.
Figure 9. FTIR spectra (a), PL spectra (b), transient photocurrent response curves under intermittent irradiation of simulated sunlight, (c) and Nyquist plots of the EIS spectra under simulated sunlight irradiation (d) of Bi4Ti3O12 and [email protected]4Ti3O12.
Figure 10. Schematic illustration of the photocatalytic mechanism of [email protected]4Ti3O12 for the dye degradation under simulated sunlight irradiation.
Figure 11. (a) Effect of ethanol, BQ and AO on the degradation percentage of RhB at 120 min of photocatalysis. (b) Mott–Schottky plot of Bi4Ti3O12 square plates obtained at 5000 Hz.
Table 1. Degradation percentage of RhB (reaction for 120 min) and apparent first-order reaction rate constant kapp for Bi4Ti3O12 and [email protected]4Ti3O12 composites under irradiation of simulated sunlight and visible light.
|Samples||Simulated Sunlight||Visible Light|
|Degradation (%)||kapp (min−1)||Degradation (%)||kapp (min−1)|
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