纳米Pb(Zr0.52Ti0.48)O3-Fe85B5Si10悬臂梁和谐振栅晶体管的巨磁电效应

Feng Li, Z. Fang, R. Misra, S. Tadigadapa, Qiming Zhang, S. Datta
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引用次数: 2

摘要

磁电(ME)层压板显示出比天然多铁材料(如Cr2O3, BiTiO)高几个数量级的ME系数。最近的研究表明,使用Fe85B5Si10 (met玻璃)/聚偏氟乙烯复合材料的体ME传感器在20 Hz时具有很高的ME电压系数21V/cm·Oe[1]。然而,大块传感器存在环氧树脂粘合不良、老化和难以与CMOS电子器件集成的问题。在这里,我们首次报道了在硅衬底上单片纳米制造Pb(Zr0.52Ti0.48)O3 (PZT)-Fe85B5Si10 ME悬臂梁(图1(a)),在20 Hz时达到0.46 V/cm·Oe,在8.4 KHz的谐振频率下达到1.8 V/cm·Oe。设计并分析了基于ME悬臂梁的谐振栅晶体管(RGT)(图1 (b))与ME悬臂梁的对比。ME RGT可使信噪比提高10倍。这显示了纳米制造悬臂式电磁传感器与硅工艺技术的兼容性,为未来基于MEMS的超灵敏磁传感器与先进的硅纳米电子学的集成铺平了道路。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Giant magnetoelectric effect in nanofabricated Pb(Zr0.52Ti0.48)O3-Fe85B5Si10 cantilevers and resonant gate transistors
Magnetoelectric (ME) laminates show higher ME coefficients than that of natural multiferroics (e.g. Cr2O3, BiTiO) by up to several orders of magnitude. Recent studies on bulk ME sensors using Fe85B5Si10 (Metglas) /polyvinylidene fluoride composite show a high ME voltage coefficient of 21V/cm·Oe at 20 Hz [1]. However, bulk sensors suffer from poor epoxy bonding, aging and difficulty of integration with CMOS electronics. Here, we report, for the first time, the monolithic nanofabrication of Pb(Zr0.52Ti0.48)O3 (PZT)-Fe85B5Si10 ME cantilevers (Fig.1(a)) on silicon substrate which achieve 0.46 V/cm·Oe at 20 Hz and 1.8 V/cm·Oe at a resonance frequency of 8.4 KHz. Also, ME cantilever based resonant gate transistors (RGT) (Fig.1 (b)) has been designed and analyzed in comparison with ME cantilever. A 10X signal to noise ratio improvement can be reached by ME RGT. This shows the compatibility of the nanofabricated cantilever ME sensors with the Si process technology and paves the way for the future integration of MEMS based ultra-sensitive magnetic sensors with advanced Si nanoelectronics.
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