Abstract

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(Zr <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">1-x</sub> Ti <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">x</sub> )O <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> (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 (α <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">ME,r</sub> ) 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.

Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call