2019
DOI: 10.1063/1.5078787
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Giant non-volatile magnetoelectric effects via growth anisotropy in Co40Fe40B20 films on PMN-PT substrates

Abstract: Uniaxial magnetic anisotropy was imposed on a CoFeB film by applying an in-plane magnetic field during growth. Electrically driven strain from a ferroelectric 0.68Pb(Mg 1/3 Nb 2/3)O 3-0.32PbTiO 3 (011) substrate resulted in giant magnetoelectric effects, whose coupling constant peaked at a record value of $8.0 Â 10 À6 s m À1. These large magnetoelectric effects arose due to non-volatile 90 rotations of the magnetic easy axis, reflecting a competition between the fixed growth anisotropy and the voltage-controll… Show more

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Cited by 31 publications
(31 citation statements)
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References 39 publications
(73 reference statements)
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“…This experiment shows that different in-plane (a1, a2) and out-of-plane (c) ferroelectric domains have a one-to-one correlation to magnetic domains with varying magnetic uniaxial anisotropy. Similar effects were observed in other ferromagnets: CoFe [72], CoFeB [73,74], Fe [75], La 1-x Sr x MnO-- 3 (LSMO) [76], Ni [77], and NiFe [78]. A key requirement for these observations is strong elastic pinning of magnetic domain walls onto ferroelectric domain walls [79].…”
Section: Controlled Ferroelectric and Multiferroic Domain Architecsupporting
confidence: 69%
“…This experiment shows that different in-plane (a1, a2) and out-of-plane (c) ferroelectric domains have a one-to-one correlation to magnetic domains with varying magnetic uniaxial anisotropy. Similar effects were observed in other ferromagnets: CoFe [72], CoFeB [73,74], Fe [75], La 1-x Sr x MnO-- 3 (LSMO) [76], Ni [77], and NiFe [78]. A key requirement for these observations is strong elastic pinning of magnetic domain walls onto ferroelectric domain walls [79].…”
Section: Controlled Ferroelectric and Multiferroic Domain Architecsupporting
confidence: 69%
“…To establish non-volatile magnetic switching for ME memory applications, symmetry-breaking mechanisms have been proposed and demonstrated. Among them are the use of competing magnetic anisotropies [190][191][192], partial poling of the piezoelectric layer [184,193,194], structural phase transitions in PMN-PT [195], ferroelastic domain switching [196], and fast strain dynamics [197][198][199]. Strain transfer from PMN-PT (or PZT [179,[200][201][202] and PZN-PT [179,190,196,203]) substrates to magnetic oxides has been shown to modify the magnetization, transition temperature, magnetoresistance, magnetic anisotropy or FMR.…”
Section: Electric-field Control Of Magnetismmentioning
confidence: 99%
“…There are three distinct ways to achieve artificial magnetoelectric coupling [5]: via (i) strain, (ii) direct (spin) exchange, and (iii) charge coupling, see section 2. In strain coupled artificial multiferroics, piezoelectric crystal or thin film and magnetostrictive layer are elastically coupled leading to controllable magnetoelastic anisotropy due to propagation of electrostrain [70,[157][158][159][160][161][162][163][164] with a key requirement of strong elastic pinning of magnetic domain walls onto ferroelectric domain walls [165]. In exchange-biased multiferroic composites, the interaction occurs between a ferromagnet and intrinsic multiferroic with uncompensated antiferromagnetic order, such as BiFeO3 [21,98,166,167], YMnO3 [168] and LuMnO3 [118].…”
Section: Domain Imprintmentioning
confidence: 99%