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Magnetoelectric Coupling in Metglas/BaTiO<sub>3</sub>/Metglas Lead-Free Magnetoelectric Composites

Magnetoelectric Coupling in Metglas/BaTiO<sub>3</sub>/Metglas Lead-Free Magnetoelectric Composites
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摘要 We report the magnetoelectric (ME) coupling in ME composites composed of NiFe<sub>2</sub>O<sub>4</sub> (NFO) or metglas as magnetostrictive phases and BaTiO<sub>3</sub> (BTO) as piezoelectric phase, targeting lead free magetnic field sensors. NFO and BTO phases were synthesized by solid state sintering method and further characterized by using XRD and FESEM techniques. The P-E hysteresis curve shows good ferroelectric behavior with saturation polarization of P<sub>s</sub> = 15.87 C/cm<sup>2</sup> and coercive electric field of 130 kV/cm. The ME response was characterized as a function of dc magnetic field at a fixed frequency. The transverse ME voltage coefficient, αME31 shows 2 times larger magnitude than that of longitudinal ME voltage coefficient, α<sub>ME31</sub>. The maximum α<sub>ME31</sub> of 37 mV/cm&bull;Oe (@H<sub>dc</sub> = 250 Oe) is observed for NFO/BTO/NFO ME composites with thickness ratio of t<sub>m</sub>/t<sub>p</sub> = 1.0. The ME coupling is further enhanced by replacing NFO layers by highly magnetostrictive metglas layers. Metglas/BTO/metglas laminates show large α<sub>ME31</sub> value of 81 mV/cm&bull;Oe at relatively lower H<sub>dc</sub> of 145 Oe. The present laminates can offer promising opportunities of engineering environmental friendly ME laminate for applications in ME devices such as energy harvester and magnetic field sensors. We report the magnetoelectric (ME) coupling in ME composites composed of NiFe<sub>2</sub>O<sub>4</sub> (NFO) or metglas as magnetostrictive phases and BaTiO<sub>3</sub> (BTO) as piezoelectric phase, targeting lead free magetnic field sensors. NFO and BTO phases were synthesized by solid state sintering method and further characterized by using XRD and FESEM techniques. The P-E hysteresis curve shows good ferroelectric behavior with saturation polarization of P<sub>s</sub> = 15.87 C/cm<sup>2</sup> and coercive electric field of 130 kV/cm. The ME response was characterized as a function of dc magnetic field at a fixed frequency. The transverse ME voltage coefficient, αME31 shows 2 times larger magnitude than that of longitudinal ME voltage coefficient, α<sub>ME31</sub>. The maximum α<sub>ME31</sub> of 37 mV/cm&bull;Oe (@H<sub>dc</sub> = 250 Oe) is observed for NFO/BTO/NFO ME composites with thickness ratio of t<sub>m</sub>/t<sub>p</sub> = 1.0. The ME coupling is further enhanced by replacing NFO layers by highly magnetostrictive metglas layers. Metglas/BTO/metglas laminates show large α<sub>ME31</sub> value of 81 mV/cm&bull;Oe at relatively lower H<sub>dc</sub> of 145 Oe. The present laminates can offer promising opportunities of engineering environmental friendly ME laminate for applications in ME devices such as energy harvester and magnetic field sensors.
作者 S. D. Patil K. Y. Rajpure A. M. Shaikh S. D. Patil;K. Y. Rajpure;A. M. Shaikh(Shivaji University, Kolhapur, India;New College, Kolhapur, India)
出处 《Journal of Materials Science and Chemical Engineering》 2016年第8期1-7,共7页 材料科学与化学工程(英文)
关键词 FERROELECTRICS MAGNETOSTRICTION Mechanical Properties PIEZOELECTRICITY Strain Ferroelectrics Magnetostriction Mechanical Properties Piezoelectricity Strain
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