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Photocatalytic splitting of water over semiconductor materials has been considered as a critical approach to achieve the aim of conversing solar energy to hydrogen energy, which is regard as potential response to the global energy crisis and environmental pollution.1-3 With the outstanding stability, good photostability, nontoxicity, and low cost, TiO2 have been chosen as a promising semiconductor photocatalyst for hydrogen generation utilizing solar energy.4,5 However, TiO2 photocatalyst is limited to the UV-light irradiation for photocatalytic activation and have no effective absorption in the visible light region (λ> 420 nm) due to a large band gap of 3.2 eV. As is well known, UV light accounts for only around 4% of the entire solar spectrum while 45% of the solar energy lie in the visible light region. Therefore, it is essential to develop novel visible-light responsive photocatalysts for water splitting with high activity and good stability as an alternative to UVactive photocatalysts.
Recently, iron-based cubic spinel semiconductor with a chemical formula of MFe2O4 (M = Ca, Mg, Ni, Cu, Zn), in which divalent ions M2+ is incorporated into the lattice of the (Fe2+Fe2 3+O4 ) group, exhibits a relatively high photocatalytic properties for H2 evolution through water oxidation reactions. 6-10 In particular, n-type semiconductor zinc ferrite (ZnFe2O4 ) with a typical Eg of about 1.9 eV show effective absorption of sunlight, high photochemical stability, high catalytic activity, good durability and low cost. Despite this, the photocatalytic activity of individual ZnFe2O4 nanoparticles is pretty poor due to the rapid recombination of photo generated charge and the large scale aggregation of nanoparticles with the ferromagnetic property. Carbon materials like graphene, reduced graphene oxide (rGO), carbon nanotube, activated carbon and carbon nonofiber are appropriate as a supporting substrate to hinder the aggregation of semiconductor nanoparticles, while its superior electrical conductivity could achieve the quick transfer of electrons and inhibit the recombination of photo-generated carries efficiently, resulting in the enhancement of the photocatalytic activity.11-16 Therefore, it is significant and meaningful to develop novel ZnFe2O4 -carbon nanocomposites with effective and enhanced photocatalytic performance for hydrogen generation.
Recently, semiconductor photocatalysts with porous, hollow and flower-like spherical structures have attracted much attention due to the excellent photocatalytic activity.17-19 . In this study, carbon-incorporated porous ZnFe2O4 nanospheres have been successfully synthesized by a facile one-step solvothermal reaction and the subsequent heat process. The phase structure and morphological information of the as-prepared photocatalysts were characterized by X-ray diffraction (XRD) and Field-emission scanning electron microscopy (FESEM). The existence of graphite-like carbon on the porous nanosphere was proved by Fourier transform infrared (FTIR) spectra, X-ray photoelectron spectroscopy (XPS) and Raman spectra. The photocatalytic activity for H2 production of the obtained ZnFe2O4 -carbon nanocomposite under visible light irradiation (λ> 420 nm) and the photogenerated electron transfer between ZnFe2O4 and graphite-like carbon were also investigated.
Experimental
Typically, Zn(NO3)2•6H2O, proper stoichiometry of Fe(NO3)3•9H2O and a desired amount of polyvinylpyrrolidone (PVP) were completely dissolved into a 30mL ethanol–ethyleneglycol (EG) mixed solution (the volume ratio of ethanol and EG is 3:7). The mixtures were uniformly mixed under continuous magnetic stirring for several minutes, and the homogeneous solution was transferred into a 50mL Teflon-lined stainless autoclave and maintained at 180 °C for 24 h. The precipitates were obtained by centrifugation separation, washed several times with deionized water and ethanol alternately, and then dried in air at 80 °C for 12h. Finally, the ZnFe2O4 -carbon nanocomposites were acquired by sintering the precipitates at 500°C for 2h under N2 atmosphere with a heating rate of 2 °C /min. The as-prepared ZnFe2O4 -carbon nanocomposites with different amounts of PVP (0.05, 0.1, 0.15 or 0.2g) were named ZFO-C1, ZFO-C2, ZFO-C3 and ZFO-C4, respectively. As a comparison, the pure ZnFe2O4 sample without adding PVP obtained in the same process is denoted as ZFO-C0. The phase structure of the obtained products were were analyzed using an X-ray powder diffractometer (XRD, D8 Advance diffractometer, Bruker Corporation, Germany) using Cu Kα (λ = 1.5419 Å). Simultaneous thermogravimetric and differential thermal analyses (TGA/DTA) of the samples were performed on a thermal analyzer (STA 8000) in air with a heating rate of 10 °C min−1The morphologies and particle sizes of the samples were observed by Field-emission scanning electron microscopy (FESEM, Zeiss SUPRA 55) and transmission electron microscopy (TEM, Tecnai G2 F20 STWIN). BET surface area and pore structure of samples were performed on a Quadrasorb SI-MP surface area and porosity analyzer. Prior to the BET analysis, the powder was degassed at 120 ◦C for 5h to remove the adsorbed H2O from the surface. FT-IR spectra were taken on a KBr disk in the frequency range of 4000- 400 cm−1 by using a FT-IR spectrophotometer (Spectrum 100). Raman spectra were recorded on a laser micro-Raman spectrometer (LabRAM HR Evolution) with the exciting wavelength at 532 nm. The chemical binding energies of the respective ions in the samples were measured using X-ray photoelectron spectroscopy (XPS) (ESCALAB 250Xi). The UV–vis diffuse reflection spectra were obtained for the dry pressed disk samples on a UV–vis spectrophotometer (Cary 5000) by BaSO4 as the reflectance sample The photoluminescence emission (PL) spectra at room temperature were characterized by a fluorescence spectrophotometer (ELS980- S2S2-stm) with a 150 W Xe lamp as the excitation source.
The photocatalytic H2 production reactions were carried out a top-irradiation-type reactor connected to a gas-closed circulation and evacuation system (AULIGHT CEL-SPH2N). The photocatalytic activity evaluation of as-prepared samples were performed by dispersing 50 mg of the photocatalysts in an aqueous solution containing CH3OH (100 mL, 10 vol%) as a sacrificial electron donor. The reaction solution was evacuated to remove the air completely prior to irradiation with a 300W xenon-lamp (CEL-HXF300) equipped with an optical UV-IR cutoff filter (λ > 420 nm). The temperature of the reaction mixture was maintained at around 6 °C by a continuous flow of cooling water. The amounts of the evolved H2 was analyzed by on line gas chromatography (GC7920) equipped with a thermal conductive detector (TCD), using N2 as the carrier gas. The H2 generation experiments were performed for 5 hours, and then the photocatalysts were separated from the mixed solution by the centrifugation process. Another aqueous solution containing CH3OH (100 mL, 10 vol%) and the separated photocatalysts were added again into the reaction vessel to start a new 5 hours cycle.
Results and Discussion
Fig.1 shows the powder X-ray diffraction (XRD) pattern of the carbon-incorporated ZnFe2O4 photocatalysts synthesized with different mass ratio of PVP. It can be seen that all of the recorded diffraction peaks could be well indexed to the cubic phase of spinel ZnFe2O4 (JCPDS NO.89-1010), and no diffraction peaks derived from any other impurities could be observed. The peaks at 2θ values of 30.05°, 35.36°, 42.85°, 53.28°, 56.67° and 62.16° can be attributed to the reflection of (2 2 0), (3 1 1), (4 0 0), (4 2 2), (5 1 1) and (4 4 0) planes, respectively. Moreover, it worth noting that no obvious peaks related to carbon are observed from the XRD patterns of ZnFe2O4 -carbon nanocomposites, and the existence of carbon on the ZnFe2O4 nanospheres were proved by other characterization methods.
The carbon content of as-prepared ZnFe2O4 -carbon nanocomposites was measured and calculated by TG-DTA analysis. Fig.2 displays the TG curve of ZnFe2O4 -C3 samples from room temperature to 800 °C during the calcination process in air. As is shown, the initial weight loss appearing between room temperature and 470 °C may be ascribed to the removal of absorbed water and organic compound. With the calcination temperatures increasing, there emerges a steep decrease of about 17.5% in mass in the range of 470–770 °C corresponding to the combustion of carbon.20 Based on the TG results, the carbon content of ZnFe2O4 -carbon samples with increasing the addition amount of PVP were determined as 6.2%, 11.7%, 17.5% and 20.1%, respectively.
Conclusions
In summary, carbon-incorporated porous ZnFe2O4 nanospheres have been successfully prepared via a simple hydrothermal route and the subsequent heat process with PVP as carbon source. FESEM observations demonstrated that the ZnFe2O4 nanospheres with porous structure and diameter in the range of 100-200nm were composed of numerous primary particles. Due to excellent electron transfer property, the presence of graphite-like carbon in the ZnFe2O4 -carbon nanocomposite exhibits an effective restraint of the recombination of the photo-excited electron–hole pairs. Compared with pure ZnFe2O4 , the photocatalytic hydrogen evolution rate of carbonincorporated ZnFe2O4 nanocomposites photocatalyst in the presence of methanol sacrificial reagent under visible light irradiation is greatly improved. Together considering the magnetic separation ability and stability, ZnFe2O4 -carbon nanospheres are a promising candidate as visible-light excited photocatalyst for photocatalytic hydrogen generation.