Nonlinear magnetoelectric effect in a ring composite heterostructure

V. I. Musatov, F. A. Fedulov, D. V. Savelev, E. V. Bolotina, L. Y. Fetisov
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Abstract

Objectives. The relevance of the study of magnetoelectric (ME) effect in ring ferromagnetic–piezoelectric heterostructures is due to the possibility of creating various ME devices having improved characteristics. A detailed investigation of the nonlinear ME effect in a ring composite heterostructure based on lead zirconate titanate (PZT) piezoceramics and Metglas® amorphous ferromagnetic (FM) alloy under circular magnetization is presented.Methods. The ME effect was measured by the low-frequency magnetic field modulation method. Excitation alternating- and constant magnetic bias fields were created using toroidal coils wound on a ring heterostructure for circular magnetization of the FM layer.Results. When excited with circular magnetic fields in a non-resonant mode, the ME ring heterostructure generates a nonlinear ME voltage of higher harmonics. The field and amplitude dependencies of the first three ME voltage harmonics were investigated. ME coefficients were obtained for the linear ME effect α(1) = 5.2 mV/(Oe·cm), the nonlinear ME effect α(2) = 6 mV/(Oe2·cm), and α(3) = 0.15 mV/(Oe3·cm) at an excitation magnetic field frequency f = 1 kHz. The maximum amplitudes of the 1st and 3rd harmonics were observed at a constant bias magnetic field H ~ 7 Oe, which is almost two times smaller than in planar PZT–Metglas® heterostructures.Conclusions. A nonlinear ME effect was observed and investigated in a ring heterostructure based on PZT piezoceramics and Metglas® amorphous FM alloy. Due to the absence of demagnetization during circular magnetization of the closed FM layer, nonlinear ME effects are detected at significantly lower amplitudes of the exciting alternating and constant bias magnetic fields as compared to planar heterostructures. The investigated ring heterostructures are of potential use in the creation of frequency multipliers.
环形复合异质结构中的非线性磁电效应
目标。环形铁磁压电异质结构中磁电效应研究的相关性是由于有可能制造出各种具有改进特性的磁电器件。本文详细研究了锆钛酸铅(PZT)压电陶瓷和metglass®非晶铁磁(FM)合金在环形复合异质结构中的非线性ME效应。方法。采用低频磁场调制法对ME效应进行了测量。利用环形线圈缠绕在环形异质结构上,形成交变偏磁场和恒偏磁场,对调频层进行环形磁化。结果。在非谐振模式下,环形异质结构在环形磁场的激励下产生高次非线性ME电压。研究了前三次电压谐波的场和幅值关系。在激励磁场频率f = 1 kHz时,得到了线性ME效应α(1) = 5.2 mV/(Oe·cm)、非线性ME效应α(2) = 6 mV/(Oe·cm)和α(3) = 0.15 mV/(Oe·cm)的ME系数。在恒定偏置磁场H ~ 7oe下,pzt - metglass®异质结构的1次和3次谐波的最大振幅几乎比平面pzt - metglass®异质结构小2倍。结论。在基于PZT压电陶瓷和Metglas®非晶FM合金的环形异质结构中观察并研究了非线性ME效应。由于在封闭调频层的圆形磁化过程中没有退磁,与平面异质结构相比,在显著较低的激励交变和恒定偏压磁场振幅下检测到非线性ME效应。所研究的环形异质结构在制造倍频器方面具有潜在的用途。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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