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High Magnetic Field Sensitivity in Ferromagnetic–Ferroelectric Composite with High Mechanical Quality Factor

In this study, composite devices were fabricated using ferromagnetic FeSiB-based alloys (Metglas) and ferroelectric ceramics, and their magnetic field sensitivity was evaluated. Sintered 0.95Pb(Zr(0.52)Ti(0.48))O(3)-0.05Pb(Mn(1/3)Sb(2/3))O(3) (PZT-PMS) ceramic exhibited a very dense microstructure w...

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Detalles Bibliográficos
Autores principales: Lee, Yong-Woo, Soh, Joon-Young, Yoo, Il-Ryeol, Cho, Jiung, Ahn, Cheol-Woo, Choi, Jong-Jin, Hahn, Byung-Dong, Cho, Kyung-Hoon
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7699316/
https://www.ncbi.nlm.nih.gov/pubmed/33228129
http://dx.doi.org/10.3390/s20226635
Descripción
Sumario:In this study, composite devices were fabricated using ferromagnetic FeSiB-based alloys (Metglas) and ferroelectric ceramics, and their magnetic field sensitivity was evaluated. Sintered 0.95Pb(Zr(0.52)Ti(0.48))O(3)-0.05Pb(Mn(1/3)Sb(2/3))O(3) (PZT-PMS) ceramic exhibited a very dense microstructure with a large piezoelectric voltage coefficient (g(31) = −16.8 × 10(−3) VmN(−1)) and mechanical quality factor (Q(m) > 1600). Owing to these excellent electromechanical properties of the PZT-PMS, the laminate composite with a Metglas/PZT-PMS/Metglas sandwich structure exhibited large magnetoelectric voltage coefficients (α(ME)) in both off-resonance and resonance modes. When the length-to-width aspect ratio (l/w) of the composite was controlled, α(ME) slightly varied in the off-resonance mode, resulting in similar sensitivity values ranging from 129.9 to 146.81 VT(−1). Whereas in the resonance mode, the composite with small l/w exhibited a large reduction of α(ME) and sensitivity values. When controlling the thickness of the PZT-PMS (t), the α(ME) of the composite showed the largest value when t was the smallest in the off-resonance mode, while α(ME) was the largest when t is the largest in the resonance mode. The control of t slightly affected the sensitivity in the off-resonance mode, however, higher sensitivity was obtained as t increased in the resonance mode. The results demonstrate that the sensitivity, varying with the dimensional control of the composite, is related to the mechanical loss of the sensor. The composite sensor with the PZT-PMS layer exhibited excellent magnetic field sensitivity of 1.49 × 10(5) VT(−1) with a sub-nT sensing limit, indicating its potential for application in high-performance magnetoelectric sensor devices.