Nonlinear magnetoelectric effect in a ring composite heterostructure

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...

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Main Authors: V. I. Musatov, F. A. Fedulov, D. V. Savelev, E. V. Bolotina, L. Y. Fetisov
Format: Article
Language:Russian
Published: MIREA - Russian Technological University 2023-10-01
Series:Российский технологический журнал
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Online Access:https://www.rtj-mirea.ru/jour/article/view/764
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author V. I. Musatov
F. A. Fedulov
D. V. Savelev
E. V. Bolotina
L. Y. Fetisov
author_facet V. I. Musatov
F. A. Fedulov
D. V. Savelev
E. V. Bolotina
L. Y. Fetisov
author_sort V. I. Musatov
collection DOAJ
description 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.
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spelling doaj-art-15a73bab15114ba1b4d596bcb8bb44282025-02-03T11:45:51ZrusMIREA - Russian Technological UniversityРоссийский технологический журнал2500-316X2023-10-01115637010.32362/2500-316X-2023-11-5-63-70394Nonlinear magnetoelectric effect in a ring composite heterostructureV. I. Musatov0F. A. Fedulov1D. V. Savelev2E. V. Bolotina3L. Y. Fetisov4MIREA – Russian Technological UniversityMIREA – Russian Technological UniversityMIREA – Russian Technological UniversityMIREA – Russian Technological UniversityMIREA – Russian Technological UniversityObjectives. 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.https://www.rtj-mirea.ru/jour/article/view/764nonlinear magnetoelectric effectcomposite heterostructuremagnetostrictionferromagnetpiezoelectric effect
spellingShingle V. I. Musatov
F. A. Fedulov
D. V. Savelev
E. V. Bolotina
L. Y. Fetisov
Nonlinear magnetoelectric effect in a ring composite heterostructure
Российский технологический журнал
nonlinear magnetoelectric effect
composite heterostructure
magnetostriction
ferromagnet
piezoelectric effect
title Nonlinear magnetoelectric effect in a ring composite heterostructure
title_full Nonlinear magnetoelectric effect in a ring composite heterostructure
title_fullStr Nonlinear magnetoelectric effect in a ring composite heterostructure
title_full_unstemmed Nonlinear magnetoelectric effect in a ring composite heterostructure
title_short Nonlinear magnetoelectric effect in a ring composite heterostructure
title_sort nonlinear magnetoelectric effect in a ring composite heterostructure
topic nonlinear magnetoelectric effect
composite heterostructure
magnetostriction
ferromagnet
piezoelectric effect
url https://www.rtj-mirea.ru/jour/article/view/764
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AT fafedulov nonlinearmagnetoelectriceffectinaringcompositeheterostructure
AT dvsavelev nonlinearmagnetoelectriceffectinaringcompositeheterostructure
AT evbolotina nonlinearmagnetoelectriceffectinaringcompositeheterostructure
AT lyfetisov nonlinearmagnetoelectriceffectinaringcompositeheterostructure