Perovskite LaFeO3/montmorillonite nanocomposites: synthesis, interface characteristics and enhanced photocatalytic activity
Perovskite LaFeO 3 /montmorillonite nanocomposites (LaFeO 3 /MMT) have been successfully prepared via assembling LaFeO 3 nanoparticles on the surface of montmorillonite with citric acid assisted sol-gel method. The results indicated that the uniform LaFeO 3 nanoparticles were densely deposited onto the surface of montmorillonite, mainly ranging in diameter from 10 nm to 15 nm. The photocatalytic activity of LaFeO 3 /MMT was evaluated by the degradation of Rhodamine B (RhB) under visible light irradiation, indicating that LaFeO 3 /MMT exhibited remarkable adsorption efficiency and excellent photocatalytic activity with the overall removal rate of RhB up to 99.34% after visible light irradiation lasting for 90 min. The interface characteristic and possible degradation mechanism were explored. The interface characterization of LaFeO 3 /MMT suggested that LaFeO 3 nanoparticles could be immobilized on the surface of montmorillonite with the Si-O-Fe bonds. The abundant hydroxyl groups of montmorillonite, semiconductor photocatalysis of LaFeO 3 and Fenton-like reaction could enhance the photocatalytic degradation through a synergistic effect. Therefore, the LaFeO 3 /MMT is a very promising photocatalyst in future industrial application to treat effectively wastewater of dyes.Nanoscale composite materials via supporting nanoparticles onto another matrix exhibit novel structure and distinguished performance in catalysis 1-5 , optics 6,7 , electronics 8,9 , and other applications 10 . The methods developed for the synthesis of nanoparticles onto the matrix mainly include precipitation 11,12 , sol-gel 13,14 , microwave-assisted synthesis 15,16 , phase transitions and hydrothermal process 17 . The matrix can disperse the nanoparticles and synergize properties, and the interface structure between phases can elicit new functional features. In recent years, the Nanocomposites with semiconductor nanoparticles assembled on substrates have received much attention for photocatalysis application, which has a very promising prospect in future industrial application of wastewater treatment 18,19 .Lanthanum ferrite (LaFeO 3 ) is an important P-type semiconductor with narrow band gaps of 2.65 eV and one of the most common perovskite type oxide. Perovskite type oxides have a general formula ABO 3 , where position A is occupied by the rare earth ion, and position B by the transition metal ion. LaFeO 3 possesses significant physical and chemical properties, and has been applied in advanced technologies such as electronic and magnetic materials 20 , solid oxide fuel cells 21 , gas sensor 22 and catalysts 23,24 . The properties of LaFeO 3 nanoparticles depend on structure, morphology, and size, which are strongly influenced by the synthesis process. Several methods have been reported for the synthesis of perovskite LaFeO 3 nanoparticles, such as sol-gel method, co-precipitation, solution combustion 25 , microemulsion 26 , hydrothermal process, thermal decomposition 27 . Among these, the sol-gel method is considered to be one of the most successful methods for synthesizing uniform and small LaFeO 3 nanoparticles in recent decades. However, the LaFeO 3 nanoparticles are easily agglomerated for high surface energy, which leads to serious decrease of the performance. One of effective solutions is dispersing the nanoparticles on the matrices, and the matrices provide heterojunctions for electrons and holes that restricted the charge recombination. Up to date, various matrices have been utilized for supporting catalyst nanoparticles, such as
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<p>mesoporous materials [28][29][30][31][32][33] , cordierite monolith 34 , TiO 2 films 35 , TiO 2 nanotube [36][37][38][39][40] , ZrO 2   41   , and clay minerals 42,43 . Among these matrices, the support materials with two dimension (2D) morphology have excellent performance enhancements for high specific surface area and favorable dispersion effect.</p><p>Montmorillonite is one of the most abundant clay mineral with natural 2D sheet-like morphology. The montmorillonite sheet consists of three layer structural units (TOTs), which is composed of a central AlO 4 (OH) 2 octahedral sheet and two SiO 4 tetrahedral sheets, and it possesses many hydroxyl groups. These hydroxyl groups and natural sheet-like morphology make montmorillonite become a promising matrix material for assembling LaFeO 3 nanoparticles. Montmorillonite has been successfully used to remove dyes from aqueous solutions 44 for its excellent adsorption capability and large specific surface area. Considering LaFeO 3 nanoparticles possess great catalytic performance in dye water treatment, it could be possible for montmorillonite supported LaFeO 3 nanoparticles to be used in organic dyes degradation in wastewater by the synergistic effect of adsorption and catalysis.</p><p>More than 0.7 million tons of synthetic organic dyes are produced annually worldwide 45 . Rhodamine B is one of cationic xanthene dyes used in printing, textile, photographic industries and fluorescent material. It not only irritates the skin, eyes and respiratory tract, but might cause carcinogenicity, reproductive and neural toxicity towards humans and animals. It is increasingly important to treat the highly colored wastewater with hazardous industrial chemical dyes efficiently. So far, the promising approaches to remove dyes from aqueous solutions mainly include adsorption engineering and photocatalysis technology 46,47 .</p><p>In this study, we first demonstrated sol-gel synthesis of perovskite LaFeO 3 /MMT via assembling LaFeO 3 nanoparticles on the surface of montmorillonite sheets. A series of LaMO 3 /MMT (M= Fe,Co,Ni) samples were synthesized in the same way for screening tests. Moreover, the photocatalytic activities of LaMO 3 /MMT were evaluated in detail by the photodegradation of RhB under visible light irradiation. The possible degradation mechanism was investigated, and the interface structure feature of LaMO 3 /MMT was characterized.</p><!><p>The TG-DSC curves of the precursor of LaFeO 3 /MMT are shown in Fig. 1a. The sample showed a slight weight loss of about 1.8% up to 108.3 °C with endothermic phenomenon, which was ascribed to the loss the physically absorbed water in the gel. A distinct exothermic peak accompanying massive weight loss of approximately 30% could be observed at 163.9 °C, which indicated the thermal transformation of citric acid. The exothermic process between 300 to 500 °C was attributed to the combustion decomposition of citric acid, and it led to a weight loss of 12.6%. With the temperature increasing, a slight loss process high than 500 °C was mainly ascribed to desorption of residual hydroxyl group. A slight exothermic peak at about 532.4 °C was caused by the gradual crystallization of LaFeO 3 . Therefore, 600 °C was chosen as the calcination temperature for preparing LaFeO 3 /MMT.</p><p>The phase and crystallinity of the samples were determined using powder XRD measurement (Fig. 1b). The XRD pattern of MMT clearly displayed a typical reflection at 2θ = 7.26° (001) for Na-montmorillonite, indicating the d 001 spacing of 1.217 nm. The diffraction peaks at 19.76°, 20.89°, 35.08° and 61.96° were corresponding to the main mineral component of Na-montmorillonite. The diffraction peaks at 26.6° was ascribed to the impurity of quartz. As for the pure LaFeO 3 , all diffraction peaks were readily indexed to the perovskite phase with an orthorhombic structure. The lattice parameters of pure LaFeO 3 were in excellent accordance with the standard powder diffraction data (JCPDS card No. 37-1493), and the average crystallite size was estimated to be 36.4 nm in diameter by the Scherrer's equation. There was no peak of LaFeO 3 phase in the XRD pattern of LaFeO 3 /MMT precursor, indicating the precursor was amorphous before calcined. The XRD pattern of LaFeO 3 /MMT presented the main diffraction peaks of montmorillonite and LaFeO 3 , and no new diffraction peaks occurred. The average crystallite size of LaFeO 3 in LaFeO 3 /MMT was 15.5 nm, which was smaller than that of pure LaFeO 3 .</p><p>The general morphologies of the samples were investigated by SEM. The front and side images of MMT indicated that montmorillonite sheets with 15~20 μ m in width and 0.5~1 μ m in thickness possessed smooth surface without contamination (Fig. 2a). The LaFeO 3 prepared by sol-gel method exhibited agglomeration of the particles with irregular shapes (Figure S1). From the SEM image and the EDS spectrum of LaFeO 3 /MMT (Fig. 2b), the LaFeO 3 nanoparticles were successfully assembled on the surface of montmorillonite sheets. It was clear that the diameter of LaFeO 3 particles on the montmorillonite sheets was less than that of pure LaFeO 3 particles, which agreed well with the XRD results. Therefore, The LaFeO 3 particles assembled on montmorillonite sheets could have larger surface area and more catalytic reaction sites. The EDS spectrum reveal that LaFeO 3 /MMT was mainly comprised of Si K (28.09 wt%), Al K (8.32 wt%), Mg K (1.52 wt%), Na K (1.48 wt%) and O K (19.82 wt%), as well as La K (29.19 wt%) and Fe K (11.57 wt%).</p><p>TEM characterization was adopted to obtain the further structural insights of MMT and LaFeO 3 /MMT. The samples for TEM had been dispersed fully in ethyl alcohol by sonicated for 30 min. It could be observed that the dispersed montmorillonite exhibited a 2D nanosheet with about 500 nm in width (Fig. 2c). The precursor of LaFeO 3 could be absorbed on the surfaces of montmorillonite nanosheets, and the LaFeO 3 crystals were generated from the precursor and assembled on the surfaces. Figure 2d showed that a large amount of LaFeO 3 particles were well dispersed on the surfaces of montmorillonite. The diameter of LaFeO 3 particles was mainly distributed around 10~15 nm, and the mean size was 12.52 nm. Therefore, it was expected that the growth of the LaFeO 3 particles could be effectively controlled to a nano-size level via the cooperation of citric acid supported on montmorillonite.</p><p>The energy band structure feature was considered as a key factor for photocatalytic activity. The samples were characterized by UV-vis diffuse reflectance spectroscopy to explore their optical properties. Figure 3a shows the UV-vis diffuse reflectance spectra of MMT, LaFeO 3 and LaFeO 3 /MMT. The LaFeO 3 and LaFeO 3 /MMT exhibited a broad absorption band in the wavelength ranging from 400 to 620 nm, which could be attributed to the electronic transition from the valance band to the conduction band. The LaFeO 3 and LaFeO 3 /MMT particles could absorb considerable amounts of visible light, which implied their potential applications as visible light driven photocatalysts. Under visible light irradiation, the photocatalyst absorbed light above 400 nm, which contributed to the formation of photogenerated electron-hole pairs. The MMT exhibited a weak absorption of visible light.</p><p>The band gap energy (E g ) could be estimated from a plot of (αhv) 2 versus photon energy (hv), where α, h and v were absorption coefficient, Planck constant and light frequency, respectively. The intercept of the tangent to the x-axis could give a good approximation of the band gap energy. The band gap energy was estimated to be about 2.15 eV for LaFeO 3 (Fig. 3b), 2.24 eV for LaFeO 3 /MMT and 3.86 eV for MMT. The values in this research were comparable with the previous results reported in literature 48 . The large band gap energy of LaFeO 3 /MMT compared with LaFeO 3 could be attributed to the less size of LaFeO 3 nanoparticles assembled on montmorillonite, which suggested that the band gap of LaFeO 3 /MMT was suitable for the photocatalytic decomposition of organic contaminants via activation by visible light irradiation.</p><p>The photocatalytic activity of LaFeO 3 /MMT was studied using the degradation of RhB as a probe reaction, and the results were compared with those of LaFeO 3 and MMT (Fig. 3c). There was minimal change in the RhB  solution without catalyst, indicating that the RhB solution could not self-decompose. RhB is hardly degraded with H 2 O 2 only (Fig. 3c). Adsorption was pre-conducted in dark for 30 min, and then photocatalysis proceeded under visible light at t = 0. In the adsorption phase, adsorption equilibrium was quickly reached and only physical adsorption was observed for the different samples. The adsorption efficiencies of MMT, LaFeO 3 and LaFeO 3 / MMT were 16.83%, 1.39% and 10.38% for RhB, respectively. The amount of RhB adsorption on the MMT was most, this phenomenon was mainly related to structure of montmorillonite. Montmorillonite was a 2:1-type clay mineral wherein each layer contained two SiO 4 tetrahedral sheet and an AlO 4 (OH) 2 octahedral sheet. The aluminum cations coordinated by hydroxyl groups was conducive to the adsorption of RhB. LaFeO 3 /MMT exhibited much higher adsorptive ability than LaFeO 3 , which was ascribed to the larger surface areas of LaFeO 3 /MMT.</p><p>With LaFeO 3 /MMT as the catalyst, the overall removal rate of RhB was up to 99.34% after visible light irradiation lasting for 90 min. For the case of LaFeO 3 , the removal rate of RhB was 97.33% via photocatalytic degradation. As for MMT, the concentration of RhB decreased by only 19.29%, which physic adsorption was dominant. However, at the beginning of 30 min under the visible light, the removal rate of RhB was 81.16% for LaFeO 3 / MMT, much higher than that for LaFeO 3 , which was only 58.96%. The LaFeO 3 /MMT had greater photocatalytic reaction rate than LaFeO 3 . Figure 3d shows the temporal evolution of the UV-vis absorption spectra of RhB solution during the photocatalytic reaction with LaFeO 3 /MMT. RhB solution shows a major absorption peak at 554 nm. Clearly, the intensity of the absorption peak gradually declined with increasing photocatalytic reaction time, which represented the concentration of RhB decreasing by degrees. There was no obvious absorption peak in the UV-vis absorption spectrum of the final degradation solution (Fig. 3d), indicating that RhB was degraded into H 2 O, CO 2 and non-toxic products 49 . It is observed that the RhB solution was almost degraded completely by LaFeO 3 /MMT in 90 min.</p><p>The photocatalytic performance of LaFeO 3 /MMT was higher than that of LaFeO 3 , which could be attributed to the specific properties of montmorillonite. The high adsorption property of montmorillonite contributed to the synergistic removal of RhB. The abundant hydroxyl groups could trap light holes and generate active hydroxyl radicals 50 . Therefore, montmorillonite with a natural sheet-like morphology was an excellent host material for photocatalysis, which could enhance the property of LaFeO 3 nanoparticles. The montmorillonite sheets could prevent LaFeO 3 nanoparticles aggregation and control the LaFeO 3 particle size effectively. The uniform and small LaFeO 3 nanoparticles were obtained on the surface of montmorillonite, which contributed to enhance the LaFeO 3 photocatalysis behavior.</p><p>The degradation mechanism for the photocatalytic reaction route of LaFeO 3 /MMT is schematically illustrated in Fig. 3e. Under the irradiation of visible light with energy greater than the threshold, the photogenerated electrons (e − ) were transferred to the conduction band (CB) from the valence band (VB) leaving the positive holes (h + ) in the VB. The electron-hole recombination was unavoidable; however, the abundant hydroxyl groups of LaFeO 3 /MMT could trap photoinduced holes to yield hydroxyl radicals (OH • ) and decrease the recombination rate of electron-hole pairs. The conduction band electrons probably reacted with oxygen molecules (O 2 ) to produce superoxide radical anions (O 2</p><!><p>), which could yield hydroxyl radicals. These hydroxyl radicals and photoinduced holes were the strong oxidizing agents to degrade RhB. The high adsorption property of LaFeO 3 /MMT could form the higher apparent concentration of RhB around the surface of catalyst, which further enhanced the photocatalytic activity.</p><!><p>The interface characteristics were characterized by Fourier transform infrared spectra (FTIR) and X-ray photoelectron spectroscopy (XPS). The FTIR spectra clearly showed the vibrational bands of MMT, LaFeO 3 and LaFeO 3 /MMT (Fig. 4a). For MMT, the bending vibration band of Si-O at 471 cm −1 and the stretching vibration band of O-Si-O at 1022 cm −1 indicated that the layered structure of montmorillonite consisted of silicon-oxygen tetrahedron. Bands close to 430, 471 and 518 cm −1 could be assigned to Si-O-Si, Si-O-Mg and Si-O-Al respectively. The obvious band at 3620 cm −1 was assigned to the -OH stretching region corresponding to the Al-O-H group. The broad band at 3453 cm −1 could be ascribed to the overlapping asymmetric and symmetric H-O-H stretching vibrations of H-bonded water, and OH bending vibration was observed at 1637 cm −1 . Meanwhile, the Fe-O stretching vibration at 559 cm −1 appeared in LaFeO 3 , which was characteristic of the octahedral FeO 6 group in the perovskite compounds. The band at 3402 cm −1 was attributed to the stretching vibration of O-H of absorbed water and hydroxyl group. The two bands at 1485 and1384 cm −1 were ascribed to the splitting of the asymmetric stretching of carbonates, indicating that La-carbonate species were formed on the surface of the LaFeO 3 particles due to exposure to the ambient atmosphere 51 . In the FIIR spectrum of LaFeO 3 /MMT, the band at 3620 cm −1 assigned to the Al-O-H group disappeared. The stretching vibration band of O-Si-O shifted to 1035 cm −1 from 1022 cm −1 , providing evidence that a chemical interaction existed between the LaFeO 3 nanoparticles and montmorillonite.</p><p>The surface elemental composition and chemical status of MMT and LaFeO 3 /MMT were studied by XPS analysis. A wide survey scan of XPS spectra was taken, and the peaks corresponding to O, Na, Mg, Al and Si in spectrum of MMT (Fig. 4b) and the peaks corresponding to La, Fe, O, C, Si and Al in spectrum of LaFeO 3 /MMT (Fig. 4c) are observed. The La, Fe, O, Si and Al elements were derived from the surface of LaFeO 3 /MMT, while the carbon peak could be attributed to adventitious carbon on the surface of sample. The XPS La 3d and Fe 2p core-level spectra revealed that the lanthanum and iron atoms were in the formal chemical valance state of + 3 in the LaFeO 3 /MMT 52 . The high-resolution spectrum of La 3d (Fig. 4d) showed two strong La peaks at 835.8 and 852.9 eV corresponding to spin-orbit splitting of 3d 5/2 and 3d 3/2 of La 3+ ions in oxide form. The binding energies of Fe 2p 3/2 and Fe2p 1/2 were observed at 711.1 and 723.8 eV (Fig. 4e), which corresponded to the core level spectra of Fe 3+ ions in their oxide form.</p><p>The high-resolution spectrum of O 1s (Fig. 4f) could be deconvolved into two peaks by Gaussian rule. The two peaks were wide and asymmetric, indicating that there were at least two kinds of O chemical states 49 . The major one corresponding to the binding energy at 531.8 eV was assigned to chemically absorbed hydroxyl oxygen species, while the shoulder one at 529.4 eV was attributed to the lattice oxygen species 53 . It could be concluded that there were abundant hydroxyl oxygen on catalyst, which was an important parameter to influence the catalytic performances in oxidation reaction. The high-resolution spectra of Si 2p and Al 2p for MMT and LaFeO 3 /MMT are shown in Figure S2. The Si 2p peak of LaFeO 3 /MMT had a slight shift compared with that of MMT, while the Al 2p peak had no obvious change. It indicated that LaFeO 3 nanoparticles might be immobilized on montmorillonite with the Si-O-Fe bonds.</p><p>The specific surface area and pore size distribution of MMT, LaFeO 3 and LaFeO 3 /MMT were measured from nitrogen adsorption-desorption isotherms. The N 2 adsorption-desorption isotherm curves of MMT and LaFeO 3 / MMT (Fig. 5a) exhibited type IV adsorption branch with a H3 hysteresis loop, which was characteristic of the mesoporous structure. However, LaFeO 3 almost had no hysteresis loop, indicating it had a small surface area. The Brunauer-Emmett-Teller (BET) specific surface area of MMT, LaFeO 3 and LaFeO 3 /MMT were 38.02, 5.37 and 13.15 m 2 g -1 , respectively. The LaFeO 3 powders had relatively small surface area due to the relatively large crystallite size and the agglomeration of the particles. Obviously, the LaFeO 3 /MMT sample had a higher specific surface area than LaFeO 3 , which could be attributed to the uniform distribution of LaFeO 3 on MMT. The pore size distribution of samples could be calculated by Barrett-Joyner-Halenda (BJH) method (Fig. 5b). The MMT had mesopores with average pore size centralizing at 3 nm, while LaFeO 3 exhibited a wide pore size distribution around 20 nm. The pore size distribution of LaFeO 3 /MMT was similar with that of LaFeO 3 , which might be because the LaFeO 3 nanoparticles covered on the surface of MMT. The large surface area of LaFeO 3 /MMT compared with LaFeO 3 could supply more adsorption and reactive sites, contributing to enhancing catalytic activity.</p><p>A series of LaMO 3 /MMT (M= Fe,Co,Ni) samples were synthesized via sol-gel method for screening tests. The XRD patterns of LaMO 3 /MMT showed that montmorillonite and perovskite phases existed in all LaMO 3 / MMT samples (Figure S3). The LaFeO 3 /MMT had the perovskite phase with an orthorhombic structure, while LaCoO 3 /MMT and LaNiO 3 /MMT had the perovskite phase with a rhombohedral structure. The crystallinity of LaNiO 3 /MMT was lower than that of LaFeO 3 /MMT and LaCoO 3 /MMT after calcined at 600 °C for 5 h. As for the La(FeCo)O 3 /MMT, La(FeNi)O 3 /MMT and La(CoNi)O 3 /MMT, the La(CoNi)O 3 /MMT possessed the highest crystallinity, which could be ascribed to the similar crystal structure of LaCoO 3 and LaNiO 3 .</p><p>Figure S4a shows the UV-vis diffuse reflectance spectra of LaMO 3 /MMT (M= Fe,Co,Ni). The all LaMO 3 / MMT samples exhibited a broad absorption band in the wavelength ranging from 400 to 620 nm, and LaCoO 3 / MMT had higher absorption intensity for visible light than LaFeO 3 /MMT and LaNiO 3 /MMT. The band gap energy of LaFeO 3 /MMT was higher than that of LaCoO 3 /MMT and LaNiO 3 /MMT (Figure S4b). The band gap energies of La(FeCo)O 3 /MMT, La(FeNi)O 3 /MMT and La(CoNi)O 3 /MMT were between that of LaFeO 3 /MMT and LaCoO 3 /MMT, it might be because all LaMO 3 phase possessed perovskite structure, and Fe, Co and Ni could replace with each other in crystal structure.</p><p>The photocatalytic activities of LaMO 3 /MMT (M= Fe,Co,Ni) were measured via the degradation of RhB, and the results are shown in Figure S5. All LaMO 3 /MMT samples exhibited good photocatalytic activity for RhB, and the LaFeO 3 /MMT possessed the highest removal rate up to 99.34%. Adsorption measurements for RhB showed that All LaMO 3 /MMT samples exhibited similar adsorption efficiencies ranging from 10% to 15%. LaFeO 3 /MMT presented better activity for RhB degradation than LaCoO 3 /MMT and LaNiO 3 /MMT. This could be attributed to the rapid decomposition of H 2 O 2 on the surface of LaCoO 3 /MMT and LaNiO 3 /MMT 54 . The LaMO 3 /MMT samples with Fe exhibited better photocatalytic activity for RhB, which could be ascribed to the synergistic effect between the semiconductor photocatalysis and Fenton-like reaction 55 .</p><p>LaFeO 3 /MMT-0.5 and LaFeO 3 /MMT-2 were synthesized via sol-gel method to explore the optimized ratio of LaFeO 3 , and the photocatalytic activities of the samples were evaluated via the degradation of RhB (Figure S6). LaFeO 3 /MMT-0.5 exhibited relatively high adsorption efficiency but low photocatalytic activity. LaFeO 3 /MMT possessed the highest removal rate with appropriate adsorption efficiency and photocatalytic activity. Therefore, considering photocatalytic activity and material cost, LaFeO 3 /MMT was chosen as the final optimized catalyst, the weight percentage of LaFeO 3 and MMT is 36.37% and 63.63% in the final LaFeO 3 /MMT catalyst, respectively.</p><p>In summary, perovskite LaFeO 3 /montmorillonite nanocomposites have been successfully synthesized via citric acid assisted sol-gel method. The uniform and small LaFeO 3 nanoparticles were supported on the surface of montmorillonite, and the montmorillonite sheets could prevent LaFeO 3 nanoparticles aggregation and control the LaFeO 3 particle size effectively. The main chemical valences of La and Fe are + 3 in the LaFeO 3 /MMT, and there are large amounts of hydroxyls on the surfaces of catalyst. With LaFeO 3 /MMT as the catalyst, the overall removal rate of RhB was up to 99.34% under visible light irradiation. The abundant hydroxyl groups could trap light holes and generate active hydroxyl radicals, and the high adsorption property of montmorillonite contributed to the synergistic removal of RhB. A series of perovskite LaMO 3 /MMT (M= Fe,Co,Ni) samples were synthesized via sol-gel method for photocatalytic degradation of RhB. The LaMO 3 /MMT samples with Fe exhibited better photocatalytic activity for the synergistic effect between the semiconductor photocatalysis and Fenton-like reaction. Therefore, the LaFeO 3 /MMT nanocomposites had prospective application to treat effectively wastewater of dyes.</p><!><p>Materials. Na  Preparation. In a typical synthesis, La(NO 3 ) 3 •6H 2 O (0.005 mol), Fe(NO 3 ) 3 •9H 2 O (0.005 mol), citric acid (0.010 mol) were dissolved in 30 mL mix-solvent (H 2 O/EtOH 1:2) to yield a homogeneous solution. The solution was stirred for 10 min and sonicated for 10 min at room temperature. 2.000 g of montmorillonite was added and the mixture suspension was stirred and heated to 70 °C until it became gel status. The precursor was obtained after the gel dried at 90 °C for 24 h. The precursor was calcined at 600 °C for 5 h with a heating rate of 2 °C/min, and the final product was marked as LaFeO 3 /MMT. Other samples were also prepared in the same way, and the material formulas were listed in Table S1. For comparison, Pure LaFeO 3 sample was prepared in the same way without montmorillonite.</p><p>Characterization. Differential scanning calorimetry (DSC) and thermogravimetry (TG) analysis was conducted at a heating rate of 10 °C/min in air atmosphere using a NETZSCH STA449C thermal analyzer. The X-ray diffraction (XRD) patterns of the samples were recorded on a DX-2700 X-ray diffractometer with Cu Kα radiation (λ = 0.15406 nm) at a scan rate of 0.02 °/s and at 40 kV and 40 mA. The morphology of the samples was observed using a JEOL JSM-6360LV scanning electron microscope (SEM) at an accelerating voltage of 5 kV, which equipped with EDS. Transmission electron microscope (TEM) images were obtained on a JEOL JEM-2100F microscope operating at 200 kV. The UV-vis diffuse reflectance spectra (UV-vis DRS) were obtained using a Shimadzu UV2450 UV-vis spectroscopy with an integrating sphere. Fourier transform infrared spectra (FTIR) of the samples were obtained between 4000 cm −1 and 400 cm −1 on a Nicolet Nexus 670 FTIR spectrophotometer using KBr pellets. X-ray photoelectron spectroscopy (XPS) measurements were performed on an ESCALAB 250 spectrometer. Nitrogen gas adsorption-desorption isotherms were obtained at 77 K using an ASAP 2020 surface area analyzer.</p><p>Photocatalytic activity evaluation. Decolorization of Rhodamine B (RhB) in aqueous solution was selected as a probe reaction to evaluate the photocatalytic activity of LaFeO 3 /MMT. A 150 W high pressure mercury lamp was used as a light source with wave length λ > 400 nm. In a typical photocatalytic experiment, 100 mg of catalyst was dispersed in 100 mL RhB aqueous solution (0.02 mmol/L). Before visible light irradiation, the suspensions were magnetically stirred in the dark for 30 min to ensure the establishment of an adsorption-desorption equilibrium among the catalyst, RhB and water. 1 mL of 3% H 2 O 2 was added into every vessel as oxidant to initiate the reaction. About 3 mL of analytical sample was drawn from the reaction suspension every 15 min, and the catalyst was removed by centrifugation. The reaction progress was monitored by measuring the absorbance (A) of the clarified solution at 554 nm using the UV-vis spectrophotometer. The degradation (%) was calculated from the formula: degradation (%) = (A 0 − A)/A 0 × 100%, where A 0 was the initial absorbance, and A was the absorbance at homologous times.</p>