Stabilization of Transition Metal Chromite Nanoparticles in Silica
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World Academy of Science, Engineering and Technology International Journal of Chemical and Molecular Engineering Vol:8, No:11, 2014 6WDELOL]DWLRQ RI 7UDQVLWLRQ 0HWDO &KURPLWH1DQRSDUWLFOHV LQ 6LOLFD 0DWUL[ Jiri Plocek, Petr Holec, Simona Kubickova, Barbara Pacakova, Irena Matulkova, Alice Mantlikova, Ivan Nemec, Daniel NiznanskyJana Vejpravova Abstract—This article presents summary on preparation and temperature. The magnetic ordering is therefore characteristic characterization of zinc, copper, cadmium and cobalt chromite by a considerable spin frustration and strongly depend on nanocrystals, embedded in an amorphous silica matrix. The the chemical order (the spinel inversion, oxygen deficit etc.) ZnCr2O4/SiO2, CuCr2O4/SiO2, CdCr2O4/SiO2 and CoCr2O4/SiO2 nanocomposites were prepared by a conventional sol-gel method and on the cation site occupancy in the spinel structure [8] under acid catalysis. Final heat treatment of the samples was carried (diamagnetic, paramagnetic or JT active), respectively. ◦ out at temperatures in the range of 900 − 1200 C to adjust the The zinc chromite is known as a frustrated antiferromagnet phase composition and the crystallite size, respectively. The resulting with a complex coplanar spin structure below the Neel´ samples were characterized by Powder X-ray diffraction (PXRD), temperature, T = 12 K [9] and it is arguably the most High Resolution Transmission Electron Microscopy (HRTEM), N Raman/FTIR spectroscopy and magnetic measurements. Formation magnetically-frustrated system known so far. At room 3+ of the spinel phase was confirmed in all samples. The average size of temperature, it has a cubic crystal structure where Cr the nanocrystals was determined from the PXRD data and by direct ions form a network of pyrochlore-like lattice [10]. The particle size observation on HRTEM; both results were correlated. Curie-Weiss temperature is about 390 K, indicating strong The mean particle size (reviewed by HRTEM) was in the range from ∼ antiferromagnetic frustration, yet chromium spins remain in 4 to 46 nm. The results showed that the sol-gel method can be T effectively used for preparation of the spinel chromite nanoparticles a cooperative paramagnetic phase down to the N. There, embedded in the silica matrix and the particle size is driven by the a first-order phase transition from a cubic paramagnet to a type of the cation A2+ in the spinel structure and the temperature tetragonal antiferromagnet signals the end of distinct spin and of the final heat treatment. Magnetic properties of the nanocrystals lattice degrees of freedom. It is a unique example of the were found to be just moderately modified in comparison to the bulk so-called spin Jahn-Teller system [11]. phases. The other example with a diamagnetic cation, the cadmium Keywords—Chromite, Fourier transform infrared spectroscopy, chromite exhibits an elliptical spiral magnetic structure below agnetic properties, nanocomposites, Raman spectroscopy, Rietveld the T = 7.8 K and simultaneously reveals a dielectric anomaly refinement, sol-gel method, spinel. N at the TN [12]. The CdCr2O4 also undergoes a spin-Peierls-like lattice distortion at the TN [13], [14]. The lattice symmetry I. INTRODUCTION is lowered from cubic to tetragonal; the lattice is elongated 2+ 3+ along the c-axis, while it shrinks in the same direction in HROMITES with A Cr2 O4 formula are binary oxides, C where A2+ and Cr3+ are cations occupying tetrahedral the ZnCr2O4. It is also surprising that the magnitude of the (A) and octahedral (B) sites, respectively. The chromites are distortion is larger in the Zn compound with weaker magnetic considered as materials with variety of potential applications interactions. 2+ ranging from high-temperature ceramics [1], catalysis [2], While less common, tetrahedral Cu on the A site semiconductors [3]–[6] to electrochemical sensors [7]. of the spinel network also displays JT activity, with the T At high-enough temperatures, the chromites crystallize relatively high JT temperature, JT = 830 K, resulting in the in a cubic structure (space group Fd-3m), with 56 atoms tetragonal structure (space group I41/amd). This distortion per unit cell (Z = 8). The 3d3 electron configuration of lowers symmetry by compressing the tetrahedron and thereby 3+ breaking the degeneracy of the partially-occupied t2 energy Cr is very stable because each of the t2g energy level is singly occupied, so there is no tendency of site mixing or levels [15]. Magnetic properties of the copper chromite have mixed valence. In the chromites with Jahn-Teller (JT) active been rarely investigated, it is reported as a hard ferromagnet International Science Index, Chemical and Molecular Engineering Vol:8, No:11, 2014 waset.org/Publication/9999702 T A2+ cations, the collective JT distortions on the A-cations with the Curie temperature, C = 135 K. 2+ 7 results in a reduction in symmetry from cubic Fd-3m to Cobalt chromite samples with magnetic Co (d ) cations develop below TC = 94 K long-range ferrimagnetic order, and tetragonal I41/amd upon orbital ordering at the transition moreover exhibits a sharp phase transition at TS =27K to J.Plocek and P.Holec are with the Institute of Inorganic Chemistry, v.v.i., the onset of long-range spiral magnetic order [16], [17]. Academy of Sciences of the CR, 250 68 Rez, Czech Republic. Magneto-capacitive measurements show that the dielectric P.Holec, I.Matulkova, I.Nemec and D.Niznansky are with the Charles University Prague, Faculty of Science, Department of Inorganic Chemistry, constant of CoCr2O4 couples to the spiral magnetic order Hlavova 2030, 128 40, Prague 2, Czech Republic. parameter, but is insensitive to the ferrimagnetic spin S.Kubickova, B.Pacakova, A.Mantlikova and J.Vejpravova are with the component [18]. Institute of Physics, v.v.i., Academy of Sciences of the CR, Na Slovance 2, 18221 Prague, Czech Republic (corresponding author J.Vejpravova to provide phone: +420-266-052-325; fax: +420-286-890-527; e-mail: [email protected]). International Scholarly and Scientific Research & Innovation 8(11) 2014 1219 scholar.waset.org/1307-6892/9999702 World Academy of Science, Engineering and Technology International Journal of Chemical and Molecular Engineering Vol:8, No:11, 2014 As is known, the magnetic properties such as saturation The size and shape of prepared nanocomposites were magnetization, remanent magnetization and coercivity, analyzed on a HRTEM JEOL JEM 3010 (High-Resolution respectively, depend strongly on the particles size and Transmission Electron Microscope). Particle size distribution microstructure of the materials. In case of the spinel was obtained by manual measurement and statistical chromites, significant change of magnetic order and hence evaluation of large-scale projected images. Elemental dielectric response is expected upon reduction of the particle composition of nanoparticles was verified by EDS size below a coherence length of the spiral component of the (Energy-dispersive X-ray spectroscopy) analysis. magnetic structure [17], [19]. Therefore it is important to use The infrared spectra were recorded on a Thermo Scientific a proper technique by which both the size and the shape of Nicolet 6700 FTIR spectrometer (2 cm-1 resolution, KBr particles can be well controlled. One of the ways to prepare beamsplitter, DTGS detector, Happ-Genzel apodization) in the nanocrystals with the required properties represents the the 400 - 4000 cm-1 region using nujol mull (KBr windows) sol-gel method [20], [21]. The advantages of this method technique. The FAR IR spectra were recorded down to 50 cm-1 are namely a good homogeneity of the final materials, low (4 cm-1 resolution, Solid SubstrateTM beamsplitter, DTGS temperatures of the treatment, and control of the particle detector, Happ-Genzel apodization) in PE pellets. size by final heat treatment. On the other hand, to stabilize The Raman spectra were recorded on a Thermo a ternary spinel phase in silica matrix, which has an acidic Scientific DXR Raman Microscope interfaced to an nature, is a challenging task. Olympus microscope (objective 50x) in the 50 - 1900 cm-1 In this work we focused on optimization of the fabrication spectral region with ∼ 3cm-1 resolution. The power of procedure in order to obtain single phase transition metal frequency-stabilized single mode diode laser (780 nm) chromite nanoparticles, embedded in the silica matrix. The impinging on the sample was ranging from 1 to 4 mW. optimized samples were investigated by varied of experimental The spectrometer was calibrated by software-controlled techniques and results of structure characterization and calibration procedure using multiple neon emission lines magnetic properties are presented. Moreover, the impact of (wavelength calibration), multiple polystyrene Raman bands the size reduction on magnetic order in selected ACr2O4 is (laser frequency calibration) and standardized white light also discussed. sources (intensity calibration). Magnetic properties were measured using a commercial 7 T - SQUID magnetometer (MPMS by Quantum Design) in the II. EXPERIMENTAL temperature range 2 - 350 K. A. Materials Preparation The conventional sol-gel method using TEOS, HNO3 III. RESULTS AND DISCUSSION as an acid catalyst, formamide as a modifier, and A. Powder X-ray Diffraction Measurement methanol as a solvent, was used for preparation of the The PXRD measurements were carried out on all samples nanocomposites. The sol was prepared by dissolving of and are shown in Fig. 1. Phase compositions (of selected the corresponding amount of the Cr(NO ) ·9H O and 3 3 2 samples) are summarized in the Table I. All samples contained the Zn(NO ) ·6H O, Cu(NO ) ·3H O, Cd(NO ) ·4H O, or 3 2 2 3 2 2 3 2 2 spinel phase, together with the other impurity phases in some Co(NO ) ·6H O, respectively, in methanol. The Si/Cr molar 3 2 2 cases, as will be discussed further. In some samples, the ratio was 5/1, which corresponds to the SiO /ACr O (where 2 2 4 shape of the spinel phase diffraction peaks with the steep A = Zn, Cu, Cd, and Co) molar ratio of 10/1.