Strain mediated magnetoelectric coupling induced in (x) Bi0.5Na0.5TiO3-(1−x) MgFe2O4 composites
Introduction
Multiferroic materials due to their scientific and technological interest have drawn much attention in last few years. These materials exhibit simultaneous presence of ferroelectricity and ferromagnetism in same phase. The most fascinating characteristic of these materials is the presence of magnetoelectric (ME) effect, which allows the coupling between ferroelectricity and ferromagnetism, implying that electric polarization can be produced by applying either an electric field or magnetic field [1], [2]. These can be used in sensors and actuators which exploit their ferroelectric and ferromagnetic properties independently, and also these are potential candidates for devices such as magnetic field sensors, multiple state memories which exploit ME coupling [3]. Multiferroic materials can be acquired in two forms: single phase and composites. The single phase multiferroics exhibit feeble ME coupling, which limits their applications in devices. The composite materials are the better alternative to these materials as high ME coupling based on the concept of product property, can be realized in these materials by taking a suitable combination of good quality piezoelectric and magnetostrictive phases [4], [5].
BNT has high Curie temperature ~330 °C [6] and shows an anomalous dielectric transition from antiferroelectric to the ferroelectric state around 200 °C. BNT is considered to be a prominent candidate for ultrasonic generators and ferroelectric random access memory (FRAM) [7]. BNT is a perovskite ABO3 type ferroelectric material. It exhibits a rhombohedral R3c polar structure at room temperature [8] and high piezoelectric constant with good electromechanical coupling factor [9].
Due to the magnetic phase in the composites, the problem of high leakage current arises in these systems, hence we choose a ferrite containing magnesium (MgFe2O4) having high specific resistance [10]. MgFe2O4 (MgFO) is an important magnetic oxide with spinel structure. Magnesium ferrite has found wide applications in microwave devices due to its lower magnetic and dielectric losses [11]. In the past years, various magnetoelectric composites such as Ni0.65Zn0.35Fe2O4-PbZr0.53Ti0.47O3 [12], CuFe2O4-PbZr0.53Ti0.47O3 [13], BaTiO3-MgFe2O4 [10], [14], [15], (x)Co0.5Zn0.5Fe2O4–(1−x)PLZT [16]. As lead (Pb)-based compounds exhibit high piezoelectric response as a ferroelectric phase, therefore in most of the composites these are taken as ferroelectric phase. But the Pb-based ferroelectric has detrimental nature with respect to living beings as well as environment, hence the lead-free ferroelectric materials have become worldwide research topic [17]. In this paper, the synthesis and characterization of (x)Bi0.5Na0.5TiO3-(1–x)MgFe2O4 composites, containing Magnesium ferrite (MgFe2O4) as the ferrite component and Bismuth sodium titanate (Bi0.5Na0.5TiO3) as the ferroelectric component has been carried out. Hence, on detailed literature survey it has been found that this system has not been reported yet. In this present work, we have investigated the structural, microstructural, dielectric, magnetic, magneto-electric and optical properties of composite of MgFO and BNT synthesized by solid state reaction (SSR) method.
Section snippets
Materials
The composites of (x)Bi0.5Na0.5TiO3-(1–x)MgFe2O4 consisting of two individual phases were prepared by solid state reaction method. For ferrite phase, stoichiometric amounts of MgO (Light LR, S.D. Fine-Chem. Ltd.) and Fe2O3 (Iron(III) Oxide, 98%, Himedia, India) were weighed and mixed in an acetone medium and calcined at 1050 °C for 2 h in air atmosphere and for ferroelectric phase, analytic grade reagents Bi2O3 (99.5%, Himedia, India), Na2CO3 (99.9%, Qualigens, India) and TiO2 (99%, Himedia,
Structural analysis
The X-ray diffraction (XRD) patterns for (x) Bi0.5Na0.5TiO3-(1−x) MgFe2O4 composites, where x=0.5, 0.6, 0.7, and 0.8 along with the individual phases of MgFO and BNT are shown in Fig. 1. It is clear from Fig. 1 that the composite systems exhibit both the parent phases i.e. spinel (ferrite) phase of MgFO (according to JCPDS Card No. 36-0398) and tetragonal perovskite (ferroelectric) phase of BNT (according to JCPDS Card No. 36-0340), with one impurity peak corresponding to Bi as denoted by (·)
Conclusions
ME composite of (x) Bi0.5Na0.5TiO3-(1−x) MgFe2O4, with x=0, 0.5, 0.6, 0.7, 0.8 and 1.0 were synthesized by the solid state reaction method. The composites were found to exhibit mixed spinel-rhombohedral phase. Average grain size as determined was found to increase from 0.62 to 2.90 µm, with the addition of BNT content. In the dielectric study with temperature an anomaly has been observed at Td, which corresponds to the ferroelectric-antiferroelectric transition of BNT. Magnetoelectric coupling
Acknowledgement
Authors would like to acknowledge the CSIR, New Delhi, India for financial support under the grant 09/143(0801)/2011-EMR-I dated 2-11-2011. One of the authors Nidhi Adhlakha. acknowledges support by the Abdus Salam International Centre for Theoretical Physics, Trieste, Italy, under the ICTP-TRIL fellowship scheme.
References (51)
- et al.
Magnetic and electrical properties of bulk BaTiO3+MgFe2O4 composite
J. Magn. Magn. Mater.
(2011) - et al.
Fine-grained BaTiO3–MgFe2O4 composites prepared by a Pechini-like process
J. Alloy. Compd.
(2015) - et al.
Composition dependent electrical, dielectric, magnetic and magnetoelectric properties of (x)Co0.5Zn0.5Fe2O4+(1-x)PLZT composites
J. Alloy. Compd.
(2010) - et al.
Structural, dielectric and piezoelectric properties of (x) BiFeO3-(1-x) BaTi0.9Zr0.1O3 ceramics
Ceram. Int.
(2014) - et al.
Enhancement of upconversion emission in Y3Al5O12:Er3+ induced by Li+ doping at interstitial sites
Chem. Phys. Lett.
(2010) - et al.
Relation of structure and magnetic properties in nickel substituted MgFe2O4
J. Magn. Magn. Mater.
(2010) - et al.
Structural, electrical and magnetic characterization of Ni–Mg spinel ferrites
J. Alloy. Compd.
(2009) - et al.
Dielectric relaxation, conductivity behavior and magnetic properties of Mg substituted Zn-Li ferrites
Curr. Appl. Phys.
(2011) - et al.
AC electrical conductivity and magnetic properties of BiFeO3–CoFe2O4 nanocomposites
J. Alloy. Compd.
(2014) - et al.
Effective dielectric and magnetic properties of (Ni–Co–Cu)ferrite/BTO composites
Mater. Chem. Phys.
(2009)
Magnetoelectric characterization of xNi0.75Co0.25Fe2O4–(1-x)BiFeO3 nanocomposites
J. Phys. Chem. Solids
Large magnetoelectric properties in CoFe2O4:batio3 core–shell nanocomposites
J. Magn. Magn. Mater.
Effect of CoFe2O4 mole percentage on multiferroic and magnetoelectric properties of Na0.5Bi0.5TiO3/CoFe2O4 particulate composites
Ceram. Int.
Comparative study of magnetoelectric composite system Ba0.95Sr0.05TiO3–Ni0.8Co0.2Fe2O4 with ferrite prepared by different methods
Ceram. Int.
Dielectric and magnetic properties of (x)CoFe2O4+(1−x)Ba0.8Sr0.2TiO3 magnetoelectric composites
Mater. Chem. Phys.
Structural, electrical, magnetic and magnetoelectric properties of composites
J. Magn. Magn. Mater.
The lock-in technique for studying magnetoelectric effect
J. Magn. Magn. Mater.
Synthesis and characterization of in situ grown magnetoelectric composites in the BaO–TiO–FeO–CoO system
Ceram. Int.
Why are there so few magnetic ferroelectrics?
J. Phys. Chem. B
Multiferroic magnetoelectric composites: historical perspective, status, and future directions
J. Appl. Phys.
Recent progress in multiferroic magnetoelectric composites: from bulk to thin films
Adv. Mater.
Magnetoelectric effect in composites of magnetostrictive and piezoelectric materials
J. Electroceram.
Effect of Zr on dielectric, ferroelectric and impedance properties of BaTiO3 ceramic
Bull. Mater. Sci.
Self-biased large magnetoelectric coupling in co-sintered Bi0.5Na0.5TiO3 based piezoelectric and CoFe2O4 based magnetostrictive bilayered composite
J. Appl. Phys.
Synthesis of bismuth sodium titanate nanosized powders by solution/sol–gel process
J. Am. Ceram. Soc.
Cited by (22)
Magnetism in titanates
2023, Defect-Induced Magnetism in Oxide SemiconductorsEnhanced performance of magnetoelectric voltage coefficient in giant magnetostrictive (Ni<inf>0.7</inf>Mg<inf>0.3</inf>Fe<inf>2</inf>O<inf>4</inf>)/piezoelectric (BaZr<inf>0.2</inf>Ti<inf>0.8</inf>O<inf>3</inf>) composites
2022, Solid State CommunicationsCitation Excerpt :It is observed that the dielectric constant decreases quickly with increasing frequency and then reaches a continuing value at higher frequencies. Hence, the worth of dielectric constant is high at low frequency region and therefore the value of dielectric constant is low at high frequency region; it demonstrates the massive dielectric dispersion behaviour was observed it was due to the Maxwell–Wagner type interfacial polarization and this is in good agreement with Koops phenomenological theory [20]. Thus, high values of dielectric constant observed at lower frequencies are explained on the idea of space charge polarization; it was due to the inhomogeneous dielectric structure of the composites.
MgFe<inf>2</inf>O<inf>4</inf>/(Ba<inf>0</inf><inf>·</inf><inf>85</inf>Ca<inf>0.15</inf>) (Zr<inf>0</inf><inf>·</inf><inf>1</inf>Ti<inf>0.9</inf>)O<inf>3</inf> lead free ceramic composite: A study on multiferroic and magnetoelectric coupling properties at room temperature
2021, Journal of Alloys and CompoundsMagnetic interaction between BHF (BaFe<inf>12</inf>O<inf>19</inf>) and BTO (BaTiO<inf>3</inf>) in BTO – BHF nanocomposite
2020, Journal of Magnetism and Magnetic MaterialsCitation Excerpt :Now-a-days, magnetic materials have drawn considerable attention of researchers due to its various applications in the field of magnetic recording ribbons, semiconductor transducers, etc. [1–3].
Magnetic properties of (1 − x)Bi<inf>0.5</inf>Na<inf>0.5</inf>TiO<inf>3</inf> + xMnTiO<inf>3</inf> materials
2019, Journal of Magnetism and Magnetic Materials