Magnetoelectric Induced Switching of Perpendicular Exchange Bias Using 30-nm-Thick Cr<sub>2</sub>O<sub>3</sub> Thin Film

Magnetoelectric (ME) effect is a result of the interplay between magnetism and electric field and now, it is regarded as a principle that can be applied to the technique of controlling the antiferromagnetic (AFM) domain state. The ME-controlled AFM domain state can be read out by the magnetization o...

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Main Authors: Yu Shiratsuchi, Yiran Tao, Kentaro Toyoki, Ryoichi Nakatani
Format: Article
Language:English
Published: MDPI AG 2021-03-01
Series:Magnetochemistry
Subjects:
Online Access:https://www.mdpi.com/2312-7481/7/3/36
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spelling doaj-fb8d844aacfa4fd8a5d3ea11e60a0b1c2021-03-10T00:04:04ZengMDPI AGMagnetochemistry2312-74812021-03-017363610.3390/magnetochemistry7030036Magnetoelectric Induced Switching of Perpendicular Exchange Bias Using 30-nm-Thick Cr<sub>2</sub>O<sub>3</sub> Thin FilmYu Shiratsuchi0Yiran Tao1Kentaro Toyoki2Ryoichi Nakatani3Department of Materials Science and Engineering, Graduate School of Engineering, Osaka University, Osaka 565-0871, JapanDepartment of Materials Science and Engineering, Graduate School of Engineering, Osaka University, Osaka 565-0871, JapanDepartment of Materials Science and Engineering, Graduate School of Engineering, Osaka University, Osaka 565-0871, JapanDepartment of Materials Science and Engineering, Graduate School of Engineering, Osaka University, Osaka 565-0871, JapanMagnetoelectric (ME) effect is a result of the interplay between magnetism and electric field and now, it is regarded as a principle that can be applied to the technique of controlling the antiferromagnetic (AFM) domain state. The ME-controlled AFM domain state can be read out by the magnetization of the adjacent ferromagnetic layer coupled with the ME AFM layer via exchange bias. In this technique, the reduction in the ME layer thickness is an ongoing challenge. In this paper, we demonstrate the ME-induced switching of exchange bias polarity using the 30-nm thick ME Cr<sub>2</sub>O<sub>3</sub> thin film. Two typical switching processes, the ME field cooling (MEFC) and isothermal modes, are both explored. The required ME field for the switching in the MEFC mode suggests that the ME susceptibility (α<sub>33</sub>) is not deteriorated at 30 nm thickness regime. The isothermal change of the exchange bias shows the hysteresis with respect to the electric field, and there is an asymmetry of the switching field depending on the switching direction. The quantitative analysis of this asymmetry yields <i>α</i><sub>33</sub> at 273 K of 3.7 ± 0.5 ps/m, which is comparable to the reported value for the bulk Cr<sub>2</sub>O<sub>3.</sub>https://www.mdpi.com/2312-7481/7/3/36magnetoelectric effectantiferromagnetismCr<sub>2</sub>O<sub>3</sub> thin filmexchange bias
collection DOAJ
language English
format Article
sources DOAJ
author Yu Shiratsuchi
Yiran Tao
Kentaro Toyoki
Ryoichi Nakatani
spellingShingle Yu Shiratsuchi
Yiran Tao
Kentaro Toyoki
Ryoichi Nakatani
Magnetoelectric Induced Switching of Perpendicular Exchange Bias Using 30-nm-Thick Cr<sub>2</sub>O<sub>3</sub> Thin Film
Magnetochemistry
magnetoelectric effect
antiferromagnetism
Cr<sub>2</sub>O<sub>3</sub> thin film
exchange bias
author_facet Yu Shiratsuchi
Yiran Tao
Kentaro Toyoki
Ryoichi Nakatani
author_sort Yu Shiratsuchi
title Magnetoelectric Induced Switching of Perpendicular Exchange Bias Using 30-nm-Thick Cr<sub>2</sub>O<sub>3</sub> Thin Film
title_short Magnetoelectric Induced Switching of Perpendicular Exchange Bias Using 30-nm-Thick Cr<sub>2</sub>O<sub>3</sub> Thin Film
title_full Magnetoelectric Induced Switching of Perpendicular Exchange Bias Using 30-nm-Thick Cr<sub>2</sub>O<sub>3</sub> Thin Film
title_fullStr Magnetoelectric Induced Switching of Perpendicular Exchange Bias Using 30-nm-Thick Cr<sub>2</sub>O<sub>3</sub> Thin Film
title_full_unstemmed Magnetoelectric Induced Switching of Perpendicular Exchange Bias Using 30-nm-Thick Cr<sub>2</sub>O<sub>3</sub> Thin Film
title_sort magnetoelectric induced switching of perpendicular exchange bias using 30-nm-thick cr<sub>2</sub>o<sub>3</sub> thin film
publisher MDPI AG
series Magnetochemistry
issn 2312-7481
publishDate 2021-03-01
description Magnetoelectric (ME) effect is a result of the interplay between magnetism and electric field and now, it is regarded as a principle that can be applied to the technique of controlling the antiferromagnetic (AFM) domain state. The ME-controlled AFM domain state can be read out by the magnetization of the adjacent ferromagnetic layer coupled with the ME AFM layer via exchange bias. In this technique, the reduction in the ME layer thickness is an ongoing challenge. In this paper, we demonstrate the ME-induced switching of exchange bias polarity using the 30-nm thick ME Cr<sub>2</sub>O<sub>3</sub> thin film. Two typical switching processes, the ME field cooling (MEFC) and isothermal modes, are both explored. The required ME field for the switching in the MEFC mode suggests that the ME susceptibility (α<sub>33</sub>) is not deteriorated at 30 nm thickness regime. The isothermal change of the exchange bias shows the hysteresis with respect to the electric field, and there is an asymmetry of the switching field depending on the switching direction. The quantitative analysis of this asymmetry yields <i>α</i><sub>33</sub> at 273 K of 3.7 ± 0.5 ps/m, which is comparable to the reported value for the bulk Cr<sub>2</sub>O<sub>3.</sub>
topic magnetoelectric effect
antiferromagnetism
Cr<sub>2</sub>O<sub>3</sub> thin film
exchange bias
url https://www.mdpi.com/2312-7481/7/3/36
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AT yirantao magnetoelectricinducedswitchingofperpendicularexchangebiasusing30nmthickcrsub2subosub3subthinfilm
AT kentarotoyoki magnetoelectricinducedswitchingofperpendicularexchangebiasusing30nmthickcrsub2subosub3subthinfilm
AT ryoichinakatani magnetoelectricinducedswitchingofperpendicularexchangebiasusing30nmthickcrsub2subosub3subthinfilm
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