Giant 2-D Magnetoelectric Effects in a Unique Magnetostrictive/Piezoelectric Heterostructure Without Interface Bonding

We develop a unique magnetoelectric (ME) heterostructure with giant 2-D ME effects by attaching magnetostrictive Metglas at the free end of a piezoelectric Pb(Zr1-xTix)O3 (PZT) cantilever, instead of interface bonding. The ME effects originate from flexural deformation of PZT plate driven by a mechanical force from Metglas. In experiments, the 1-D ME heterostructures induced different directional magnetic fields have been designed optimally. When the length of Metglas ribbon is 12 mm, the 1-D ME heterostructures have the maximum ME effects. After assembling the different optimal designed 1-D ME heterostructures, an ME heterostructure with 2-D ME characteristics is obtained. The 2-D heterostructure has two resonant frequencies, at about 88 and 115 kHz. The maximum resonant voltage coefficient (αME,r) is 79 (V/cm Oe) when the heterostructure is in one direction of the magnetic field, and 45 (V/cm Oe) when the heterostructure is in the other direction of the magnetic field. The results demonstrate that this ME structure can be used as a multidimensional ME transducer.

[1]  C. Nan,et al.  Multiferroic Magnetoelectric Composites: Historical Perspective, Status, and Future Directions , 2008, Progress in Advanced Dielectrics.

[2]  Jitao Zhang,et al.  Zero-biased magnetoelectric composite Fe73.5Cu1Nb3Si13.5B9/Ni/Pb(Zr1−x,Tix)O3 for current sensing , 2014 .

[3]  Jitao Zhang,et al.  Dynamic magnetostrictive properties of magnetization-graded ferromagnetic material and application in magnetoelectric composite , 2014 .

[4]  D. Viehland,et al.  Giant magnetoelectric effect in self-biased laminates under zero magnetic field , 2013 .

[5]  Miao Yu,et al.  Investigation of magnetostrictive/piezoelectric multilayer composite with a giant zero-biased magnetoelectric effect , 2013 .

[6]  Y. Wen,et al.  Magnetoelectric Transducer Employing Piezoelectric Ceramic/Ferromagnetic Alloy/High-Permeability FeCuNbSiB Composite , 2011, IEEE Transactions on Magnetics.

[7]  G. Lawes,et al.  Introduction to magnetoelectric coupling and multiferroic films , 2011 .

[8]  D. Pan,et al.  Large magnetoelectric effect in mechanically mediated structure of TbFe2, Pb(Zr,Ti)O3, and nonmagnetic flakes , 2011, 1210.7542.

[9]  C. Nan,et al.  Recent Progress in Multiferroic Magnetoelectric Composites: from Bulk to Thin Films , 2011, Advanced materials.

[10]  R. Ramesh,et al.  Magnetoelectric Coupling Effects in Multiferroic Complex Oxide Composite Structures , 2010, Advanced materials.

[11]  G. Srinivasan,et al.  Enhancement of magnetoelectric coupling in a piezoelectric-magnetostrictive semiring structure , 2009 .

[12]  贾艳敏 Bidirectional current-voltage converters based on magnetostrictive/piezoelectric composites , 2009 .

[13]  Siu Wing Or,et al.  Giant magnetoelectric effect in mechanically clamped heterostructures of magnetostrictive alloy and piezoelectric crystal-alloy cymbal , 2008 .

[14]  Ping Li,et al.  Enhanced magnetoelectric effects in composite of piezoelectric ceramics, rare-earth iron alloys, and ultrasonic horn , 2007 .