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Converse magnetoelectric effect in laminated composites of PMN–PT single crystal and Terfenol-D alloy

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5 Author(s)
Jia, Yanmin ; Department of Applied Physics, The Hong Kong Polytechnic University, Hung Hom, Kowloon, Hong Kong and State Key Laboratory of High Performance Ceramics and Superfine Microstructure, Shanghai Institute of Ceramics, Chinese Academy of Sciences, 215 Chengbei Road Jiading, Shanghai 201800, China and Graduate School of the Chinese Academy of Sciences, Beijing 10039, China ; Or, Siu Wing ; Chan, H.L.W. ; Zhao, Xiangyong
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Your organization might have access to this article on the publisher's site. To check, click on this link:http://dx.doi.org/+10.1063/1.2212054 

We have found experimentally and theoretically that laminated composites comprising one layer of length-magnetized Tb0.3Dy0.7Fe1.92 (Terfenol-D) magnetostrictive alloy sandwiched between two layers of thickness-polarized, electro-parallel-connected 0.7Pb(Mg1/3Nb2/3)O3–0.3PbTiO3 (PMN–PT) piezoelectric single crystal have a large converse magnetoelectric effect characterized by a large magnetic induction in response to an applied ac voltage. The reported converse magnetoelectric effect originates from the product of the converse piezoelectric effect in the PMN–PT layers and the converse magnetostrictive effect in the Terfenol-D layer. Large converse magnetoelectric coefficient in excess of 105 mG/V is obtained in the composites at a low magnetic bias field of 170 Oe. The measured magnetic induction has an excellent linear relationship to the applied ac voltage with amplitude varying from 50 to 160 V. These made the composites to be a promising material for direct realization of core-free magnetic flux control devices.

Published in:
Applied Physics Letters  (Volume:88 ,  Issue: 24 )

Date of Publication: Jun 2006

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