Detection of para–antiferromagnetic transition in Bi2Fe4O9 powders by means of microwave absorption measurements
Introduction
Bi2Fe4O9 compound is known to have an orthorhombic structure [1], [2], see Fig. 1, where the iron ions are evenly distributed between the tetrahedral and octahedral positions with the bismuth ions surrounded by eight oxygen atoms. But also, it can be described by columns of edge-sharing FeO6 octahedra parallel to the c axis, bonded by corner-sharing FeO4 tetrahedra and Bi atoms. This bismuth ferrite material is generally synthesized by a traditional solid-state reaction at temperature over 850 °C [2], [3]. However, because of some disadvantages of this method such as high temperature, the presence of impurities in the compounds and largesize of particles, other synthesis methods have also been employed; e.g. Park et al. [4] have used a molten salt technique for the synthesis of submicron-sized Bi2Fe4O9 cubes using Bi2O3 and Fe2O3 as starting materials.
Additionally, concerning the application, it is important to say that Bi2Fe4O9 compound is an important material that can be used for a semiconductor gas sensor and catalyst for ammonia oxidation to NO [5], [6]. This compound shows a para–antiferromagnetic transition around 240–265 K [3], [7], in which the magnetic ordering is due to superexchange interaction between the Fe ions mediated by the O atoms. Singh et al. [3] reported remarkable multiferroic effects in polycrystalline Bi2Fe4O9 which exhibits an antiferromagnetic ordering and ferroelectric hysteresis. Therefore, Bi2Fe4O9 is a promising multiferroic material.
The electron paramagnetic resonance (EPR) is the most powerful spectroscopic method available to unambiguously determine the valence state of paramagnetic ions [8], as well as to determine the local structural information and symmetry of paramagnetic ions incorporated in the structure [9], [10]. This technique also allows the investigation of the nature of magnetic phases in multiferroic materials at different temperatures [11], [12], [13], [14].
On the other hand, recently, the microwave absorption around zero magnetic field (low-field microwave absorption, LFMA) has also been used to study multiferroic materials [12], [13], [14], [15]. A complementary method particularly well adapted to study magnetic transitions is the magnetically modulated microwave absorption spectroscopy (MAMMAS) [12], [15], [16], [17]. The MAMMAS technique is based on the temperature variations of the modulated microwave absorption, and provides valuable information about the nature of magnetic ordering [17].
To our knowledge, however, studies on the polycrystalline Bi2Fe4O9 with EPR, MAMMAS and LFMA techniques are scarce. Therefore, in this work, we present a detailed study of the changes in lineshape of the EPR spectra in Bi2Fe4O9 powders; these changes are quantified by means of the following parameters: the peak-to-peak linewidth (ΔHpp) and the resonant field (Hres) as a function of temperature, through para–antiferromagnetic transition. MAMMAS and LFMA techniques are used to give a further knowledge on the magnetic behavior of this material; these techniques give evidence of the magnetic transition and a weak ferromagnetism at low temperature.
Section snippets
Samples preparation and experimental techniques
The Bi2Fe4O9 powders are prepared by molten salt technique [4]. Stoichiometric amounts of Bi2O3 (Aldrich, 99.99%) and Fe2O3 (Baker, 99.9%) were mixed (in molar ratio of 1:2) with acetone and ground in an agate mortar. To this oxides mixture is added a salts mixture in the molar ratio of 1:5, where the salts mixture has the composition of Na2SO4 (37.5% mol) and Li2SO4 (62.5% mol). The powders were placed in an alumina crucible, heated at a ramp rate of 10 °C/min up to an annealing temperature at 800
Results and discussion
XRD pattern of the polycrystalline sample of Bi2Fe4O9 is shown in Fig. 2. All observed reflection lines are indexed with the orthorhombic structure of space group Pbam, in a good agreement with the standard data of the Bi2Fe4O9 powders (JCPDS Card no.: 25-0090). Additionally, in Fig. 3(a), we show the scanning electron microscopy (SEM) image, revealing the morphology of the Bi2Fe4O9 powders. It can be observed that the Bi2Fe4O9 product mainly consists of particles clusters with cubic
Conclusions
The changes in ΔHpp and Hres in the EPR spectra for Bi2Fe4O9 powders, within the region between 350 K and 200 K, can be interpreted in terms of the para–antiferromagnetic transition. At low temperature a weak ferromagnetism is observed in this material, and it is attributed to canting of Fe3+ ion sublattices in the antiferromagnetic matrix. Additionally, MAMMAS and LFMA measurements also give evidence of the magnetic ordering and also suggest a weak ferromagnetism at low temperature, with a very
Acknowledgments
G. Alvarez acknowledges research support in the laboratory of magnetic mensurations and biophysics of ESFM-IPN-Mexico. Support from project PAPIIT-UNAM No. IN111111 is gratefully acknowledged.
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