C. Y.
Lu
*ab,
T.
Puig
b,
X.
Obradors
b,
S.
Ricart
b and
J.
Ros
a
aDepartament de Quimica, Edifici C Facultat de Ciències, Universitat Autònoma de Barcelona (UAB), Cerdanyola del Vallès, Barcelona 08193, Spain. E-mail: lu.changyong@e-campus.uab.cat
bInstitute of Materials Science of Barcelona (ICMAB-CSIC), Campus de la UAB, Cerdanyola del Vallès, Barcelona 08193, Spain
First published on 12th September 2016
A novel microwave-assissted reverse microemulsion method was applied to prepare Fe3O4@SiO2 core–shell nanoparticles rapidly for the first time. The morphology of the core–shell structure is controlled by tunning the reaction parameters. Nanoparticles with a very thin SiO2 coating layer (2.5 nm) containing a single Fe3O4 nanoparticle (8–9 nm) are produced. These core–shell nanoparticles can be used as solid catalytic supports for Ag nanoparticles and applied in 4-nitroaniline reduction. Transmission electron microscopy showed that the core–shell nanoparticles were decoracted with Ag nanoparticles of 7 nm in diameter. The crystal structures of the Fe3O4 and Ag nanoparticles were confirmed by X-ray diffraction. These Ag/Fe3O4@SiO2 nanocomposites showed high catalytic efficiency and recycling properties even after 20 times of repetation.
Because of the multifunctional requirement, Fe3O4/Ag composite materials with the combination of excellent magnetic properties, biocompatibilities and plasmonic properties would be a promising composite for multiple applications. However the uncovered Fe3O4 NPs were easy to oxidized and aggregated during the preparation and application process. The chemical and thermal stable silica layers could be a nice candidate for decorating and protect the iron oxide nanoparticles' surface. And the nontoxic silica provides Fe3O4 nanoparticles with water solubility as well as good biocompatibility, which has potential applications in bio-imaging and drug delivery.8 For the research in functional materials, Fe3O4@SiO2@Y2O3:Eu3+ core–shell structures have magnetic response performance and luminescent properties9 and the Fe3O4@SiO2@Au core–shell microspheres exhibit an enhancement ability of surface-enhanced Raman scattering for rhodamine-b detection.10
Nowadays, Stöber method11–16 and reverse microemulsion system17–24 were both widely used to prepare Fe3O4@SiO2 core–shell structures. Fe3O4@SiO2 core–shell nanoparticles with ultra-thin silica shell (∼2 nm) and a high saturated magnetization (15 emu g−1)25 can be synthesized through reverse microemulsion method.26–28 However, both methods requires long time for SiO2 condensing, taking around 24 h for one reaction.29 This is a great disadvantage that hinders the fast and massive production of Fe3O4@SiO2 core/shell nanoparticles and their wide application.
Microwave irradiation significantly accelerates the reaction rate, increases yields and reduces side reactions in the preparation of different kinds of nanoparticles, from metals to oxides and semiconductors.30–32 The synthesis of NPs@SiO2 core–shell structure were only reported by using microwave assistance Stöber method,33,34 and the fast preparation of core–shell nanoparticles with controllable small size and very thin SiO2 layer remain challenging. The combination of microwave irradiation and reverse microemulsion method has the possibility to overcome this problem, to our knowledge, this method was used until now to prepare Au NPs, zincophosphates,35 MOF36 and zeolite nanocrystals37 and the results indicate that this method has great improvement on yield, size distribution and reducing the reaction than the normal reverse microemulsion method.
In this work, we report a novel rapid approach based on microwave assisted reverse microemulsion process to synthesize Fe3O4@SiO2 core–shell nanoparticles with a very thin SiO2 layer (2.5 nm in average) within only 5 min (Fig. 1). The synthesized core–shell structures were stable in ethanol and well-formed. Moreover these Fe3O4@SiO2 core–shell nanoparticles were further functionalized with (3-aminopropyl)triethoxysilane (APTES) and decorated with Ag nanoparticles. The morphology and crystal structure of Fe3O4@SiO2 and Fe3O4@SiO2/Ag nanoparticles were analysed through different techniques for example transmission electron microscopy (TEM), high resolution transmission electron microscopy (HR-TEM) and X-ray diffraction (XRD) and the magnetic properties were measured by superconducting quantum interference device (SQUID). The catalytic efficiency and recycling test were done via monitoring the 4-nitroaniline reduction reaction. The morphology of nanoparticles, such as the aggregation and the number of core particles, can be well manipulated through changing the amount of reactants. This kind of core–shell nanoparticle is superparamagnetic with a relatively high saturation magnetization value 32.7 emu g−1.27 This kind of core–shell nanoparticle could be used as the support for Ag nanoparticles and the synthesized Fe3O4@SiO2/Ag nanocomposites show great catalytic and recycling properties.
Transmission electron microscope (TEM) and high resolution transmission electron microscopy (HR-TEM) measurements were conducted on a JEOL 1210 TEM microscopy at 130 kv and a JEM-2011 HR-TEM microscopy at 200 kv. One drop of the hexane suspension of Fe3O4 nanoparticles and ethanol suspension of Fe3O4@SiO2 and Fe3O4@SiO2/Ag nanoparticles were deposited on the carbon-coated copper grids respectively. In order to minimize the aggregation of nanoparticles, the copper grids were laid on a filter paper during the drying process.
X-ray powder diffraction studies (XRD) were performed on D5000 Siemens X-ray powder diffractionmeter in a reflection mode by using Cu Kα λ = 1.5406 Å radiation in a range of 10° ≤ 2θ ≤ 80°.
The field-dependent magnetization curves were characterized by SQUID (Quantum design MPMS XL-7T) under a magnetic field from 0 to ±70000 Oe at 5 K.
The thermogravimetric analysis (TGA) was carried on a NETZSCH-STA 449 F1 Jupiter thermal analysis system from room temperature to 800 °C under a O2 flow.
Particle size distribution tests were implemented on a Zetasizer Nano Z system from Malvern Instruments (He–Ne laser 633 nm, Max 4 mW) by dynamic light scattering.
The catalytic reaction was characterized by a Varian Cary 5000 UV-Vis-NIR spectrophotometer operated at 1 nm resolution using freshly made solution in quartz cuvettes with 10 mm path length.
In the FT-IR curve of Fe3O4 nanoparticles (Fig. 3b red line), the absorption peaks at 2192 cm−1, 2850 cm−1 are attributed to –CH2 stretching vibration and 1708 cm−1 is coming from CO stretching modes of dimeric COOH groups and the peaks at 1406 cm−1 could be ascribed to the coupling of hydroxyl bending vibration with C–O stretching vibration. The absorption band at 1598 cm−1 is the characteristic peak of C
C vibration and the peak at 1522 cm−1 is belonging to the COO− asymmetric stretching vibration. All those peaks indicate that the oleic acid is absorbed on the Fe3O4 nanoparticles which results in a well dispersion of Fe3O4 in hexane. After the microwave irradiation, the FT-IR curve of Fe3O4@SiO2 (Fig. 3b black line) shows two small peaks in 1512 cm−1, 1457 cm−1 coming from stretching vibration of aromatic ring C
C and two strong peaks in 1200 cm−1 and 1060 cm−1 which attribute to the symmetric stretching vibration of
C–O–C and asymmetric stretching vibration of
C–O–C. The existence of those vibration models indicates that there are still some amounts of Igepal CO-520 attached on the nanoparticles' surface. The absorption bands at 1145 cm−1, 953 cm−1, 819 cm−1 attribute to the vibration models of SiO2 which means that the SiO2 were successfully covered on the Fe3O4 nanoparticles. The FT-IR results indicate the substitution of oleic acid and oleylamine capping ligands for the silica shell after microwave process. Strong bands centered at 820 cm−1 can be unequivocally attributed to the vibration modes of SiO2.
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Fig. 3 TEM image of Fe3O4 NPs (a) and FT-IR curve of Fe3O4 nanoparticles, Fe3O4@SiO2 core–shell nanoparticles and Fe3O4@SiO2-APTES nanoparticles (b). |
TEM studies of Fe3O4@SiO2 core–shell nanoparticles prepared with microwave assistance and normal reverse microemulsion methods (Fig. 4a and b) prove that the core–shell structure is obtained through both methods but the size of samples are significantly different: the shell thickness is 6.6 nm and total size is about 30 nm for the normal reverse microemulsion method, on the other hand the shell is only 2.5 nm thick and total size is about 14 nm for the microwave assisted reaction. The thinner shell of microwave irradiation method could be ascribed to the short irradiation time during the TEOS hydrolysis reaction. It is worth to mention that the synthesized core–shell nanoparticles are not porous which made them unable combine the multifunctional capping agents with highly loading percentage compare to the recent reports about mesoporous silica nanocarriers.39,40
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Fig. 4 TEM images of Fe3O4@SiO2 core–shell nanoparticles prepared by microwave irradiation (a) and normal reverse microemulsion process (b). |
In order to optimize the silica shell formation, different concentrations of ammonia (71 mM, 141 mM, 211 mM and 280 mM) were used in each reaction. The TEM images (Fig. 5a–d) of core–shell nanoparticles show that after the microwave process a 2–3 nm thickness shell was formed. As is presented in Fig. 4 ammonia concentrations up to 211 mM give dispersions of particles with a chain like structure. Progressive increase of the amount of ammonia produced an improvement the dispersion reaching monodisperse core–shell NPs with ammonia concentration to 280 mM (Fig. 5d). DLS studies (Fig. 6) indicate that the samples prepared by using 71 mM and 141 mM ammonia show big aggregation and the sample synthesized by adding 211 mM ammonia shows a mixture of relative small size nanoparticles and big size aggregation. When 280 mM ammonia was used in the reaction, the DLS result (Fig. 6) shows that most of core–shell nanoparticles are about 15 nm which is in agreement with TEM results (Fig. 5). This effect can be explained by the role of ammonia in decorating the condensed SiO2 surface that results in a more negatively charged layer, leading to a better dispersion of Fe3O4@SiO2 nanoparticles. It should be pointed out that in this method the increasing concentration of ammonia does not affect the shell thickness of nanoparticles (see Table 1), whereas the shell thickness were changed with different concentration of ammonia in conventional reverse microemulsion method (see Table S1, ESI†). This effect might come from the short reaction time and ammonia evaporation during the microwave irradiation. The controll of shell thickness is under study.
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Fig. 6 Particle size distribution of Fe3O4@SiO2 core–shell nanoparticles prepared under different concentration of ammonia. |
Concentration of ammonia | 71 mM | 141 mM | 211 mM | 280 mM |
Shell thickness | 2.51 nm | 2.55 nm | 2.54 nm | 2.60 nm |
The effect of the amount of surfactant was also studied. Increasing the amount of surfactant (Igepal CO-520) in the reaction produced a progressive decrease of the number of nanoparticles in the core (see Fig. 7a–c) and finally single-core core–shell nanoparticles were achieved using 400 mM surfactant. Based on the chemical mechanism previously discussed by Wang et al.,20 the molar ratio of water and surfactant (Igepal CO-520 in our case) is very important for the morphology and particle size of core–shell structures. The increase of water/surfactant ratio produces the increase of micelles size facilitating intermicellar nucleation processes. For this reason, there were more nanoparticles inside the core of the sample than the other samples when 200 mM of Igepal CO-520 was employed at the first step of micelle formation.
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Fig. 7 TEM images of Fe3O4@SiO2 core–shell nanoparticles prepared with different concentration of Igepal CO-520 inside, 200 mM (a), 300 mM (b) and 400 mM (c). |
Fe3O4@SiO2 core–shell nanoparticles prepared by microwave irradiation display a strong magnetism that allows their separation from the solution with a magnet. Fig. 8 shows the magnetization test of Fe3O4 and Fe3O4@SiO2 core–shell nanoparticles. Magnetite nanoparticles are superparamagnetic with a high saturation magnetization value (96.9 emu g−1). After covered by silica shell, the nanoparticles display a lower saturation magnetization (32.7 emu g−1) but the core–shell structure remains superparamagnetic. Based on the calculation of weight percentage (ESI†) of Fe3O4 in the core–shell structure, the magnetization of Fe3O4 nanoparticles didn't change to nonmagnetic phase during the reaction. The magnetic properties of as prepared core–shell nanoparticles are comparable to other reported in the literature.20
The magnetic materials were widely used as the support for catalysis. For example, palladium catalysts were loaded on the Ni MOF-derived N-doped magnetic mesoporous carbon for the hydrodechlorination reaction of chlorophenols.41 In this paper silver nanoparticles were synthesized on the surface of Fe3O4@SiO2 core–shell nanoparticles. The obtained core–shell nanoparticles were first functionalized with –NH2 group (see Fig. 3b blue line) by using APTES molecule. The weak absorption peaks between 1490 cm−1 and 1631 cm−1 and at 3352 cm−1 attribute the NH2 group of APTES and the peaks at 2922 cm−1 and 2852 cm−1 coming from the propyl chain of APTES molecule, all these peaks indicate the successful functionalization of –NH2 group on the surface of core–shell nanoparticles. The silver nanoparticles were formed and decorated on the surface of silica shell through a simple reduction reaction. The XRD pattern of Ag/Fe3O4@SiO2 nanocomposites (Fig. 2) indicates that strong diffraction peaks which identify with the standard Ag diffraction pattern (JCPDS no.04-0783) showing the characteristic (111), (200), (220) and (311) peaks. Fig. 9 shows the TEM images of Ag/Fe3O4@SiO2 nanoparticles. From the images, the well-dispersed sliver nanoparticles were found to attach to the surface of core–shell nanoparticles with an average diameter about 7 nm. It is noteworthy that the shell thickness of silica is thicker than the pictures in Fig. 7 which could be attributed to the process of functionalization the shell with APTES. The high angle annular dark-field scanning TEM (HAADF-STEM) image and corresponding elements mapping images (Fig. S5 ESI†), confirmed the Fe atoms were only distributed in the core and the Si atoms were homogeneously distributed around the Fe3O4 core, indicated a clearly core–shell structure. In the mean while the Ag atoms were main distributed outside the SiO2 shell suggested a successfully decoration of Ag nanoparticles on the surface of Fe3O4@SiO2 core–shell nanoparticles.
The decoration of silver nanoparticles on the Fe3O4@SiO2 core–shell structure causes a further decrease in the magnetic saturation value to 18.2 emu g−1 (Fig. 8), which was attribute to the mass effect of silver and silica. The Ag/Fe3O4@SiO2 nanocomposites showed a strong magnetization which makes it separated by external magnetic field (see Fig. 8 insert image), indicates that this nanocomposites are suitable for magnetic separation and targeting.
The principal of the reduction reaction of 4-nitroaniline to 4-phenylenediamine when using Ag/Fe3O4@SiO2 nanocomposite as the catalysis is showed in Fig. 10. This reaction is considered quite useful in the synthesis of rubber and polymer product42,43 and the catalytic reduction of nitro-compound is well studied.44 The whole reduction reaction could be easily monitored by the UV-vis spectroscopy through the decrease if the strong absorption peaks at 380 nm which could be attribute to 4-nitroanilinate anion. In the Fig. 11, a dramatically decreased of absorption peak at 380 nm when using Ag/Fe3O4@SiO2 as the catalysis, meaning while a peak at 240 nm was appeared and getting stronger with the increase of reaction time which related to the 4-phenylenediamine. Based on the previous report, the reduction reaction happened through the transfer of electrons from the 4-nitroaniline molecules as long as both compounds attached on the surface of Ag/Fe3O4@SiO2 nanocomposites. When the electron transferred to Ag nanoparticles the hydrogen atoms formed and attacked the 4-nitroaniline molecules leading to the occurrence of reduction reaction.45 It is noteworthy that the 4-nitroaniline could be fully reduced within 5 min when using our synthesized Ag/Fe3O4@SiO2 nanocomposites as the catalysis. This phenomenon could be explained by the high surface activity of Ag nanoparticles and the large surface area provided by the small size core–shell nanoparticles. These two characters ensure the Ag/Fe3O4@SiO2 nanocomposites have a good catalytic property. And the TOF value was also calculated to 6 h−1.
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Fig. 10 Reaction mechanism about the reducing 4-nitroaniline when using Ag/Fe3O4@SiO2 nanocomposites as the catalysts. |
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Fig. 11 UV-visible spectra for the reaction of 4-nitroaniline molecule by Ag/Fe3O4@SiO2 nanocomposites at various times. |
Another advantage of our synthesized Ag/Fe3O4@SiO2 nanocomposite is high recyclability compared to the single Ag nanoparticles catalysts. The recycling test of Ag/Fe3O4@SiO2 catalysis demonstrated that about 86% of 4-nitroaniline was reduced even after 20 cycles (see Fig. 12). It is worth to note that the nanoparticles start to aggregate after 20 cycles (Fig. S6†) and there were still many Ag nanoparticles located outside the aggregates. The unique core–shell structure makes the nanocomposites highly stable and easily separated by magnet results in a quite well reutilization property compared to other similar studies.46
Footnote |
† Electronic supplementary information (ESI) available: Electron diffraction pattern, thermal gravity cure, weight percentage calculation and elements mapping test. See DOI: 10.1039/c6ra19435d |
This journal is © The Royal Society of Chemistry 2016 |