Role of CoFeB thickness in electric field controlled sub-100 nm sized magnetic tunnel junctions

We report a comprehensive study on the role of the free layer thickness (tF) in electric-field controlled nanoscale perpendicular magnetic tunnel junctions (MTJs), comprising of free layer structure Ta/Co40Fe40B20/MgO, by using dc magnetoresistance and ultra-short magnetization switching measurement...

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Main Authors: James Lourembam, Jiancheng Huang, Sze Ter Lim, Ernult Franck Gerard
Format: Article
Language:English
Published: AIP Publishing LLC 2018-05-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/1.5006368
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spelling doaj-f34dee96105a43f2a0a8f66dfb105cf92020-11-24T21:17:50ZengAIP Publishing LLCAIP Advances2158-32262018-05-0185055915055915-610.1063/1.5006368114892ADVRole of CoFeB thickness in electric field controlled sub-100 nm sized magnetic tunnel junctionsJames Lourembam0Jiancheng Huang1Sze Ter Lim2Ernult Franck Gerard3Data Storage Institute, 2 Fusionopolis Way, 138634, SingaporeData Storage Institute, 2 Fusionopolis Way, 138634, SingaporeData Storage Institute, 2 Fusionopolis Way, 138634, SingaporeData Storage Institute, 2 Fusionopolis Way, 138634, SingaporeWe report a comprehensive study on the role of the free layer thickness (tF) in electric-field controlled nanoscale perpendicular magnetic tunnel junctions (MTJs), comprising of free layer structure Ta/Co40Fe40B20/MgO, by using dc magnetoresistance and ultra-short magnetization switching measurements. Focusing on MTJs that exhibits positive effective device anisotropy (Keff), we observe that both the voltage-controlled magnetic anisotropy (ξ) and voltage modulation of coercivity show strong dependence on tF. We found that ξ varies dramatically and unexpectedly from ∼−3 fJ/V-m to ∼−41 fJ/V-m with increasing tF. We discuss the possibilities of electric-field tuning of the effective surface anisotropy term, KS as well as an additional interfacial magnetoelastic anisotropy term, K3 that scales with 1/tF2. Voltage pulse induced 180° magnetization reversal is also demonstrated in our MTJs. Unipolar switching and oscillatory function of switching probability vs. pulse duration can be observed at higher tF, and agrees well with the two key device parameters — Keff and ξ.http://dx.doi.org/10.1063/1.5006368
collection DOAJ
language English
format Article
sources DOAJ
author James Lourembam
Jiancheng Huang
Sze Ter Lim
Ernult Franck Gerard
spellingShingle James Lourembam
Jiancheng Huang
Sze Ter Lim
Ernult Franck Gerard
Role of CoFeB thickness in electric field controlled sub-100 nm sized magnetic tunnel junctions
AIP Advances
author_facet James Lourembam
Jiancheng Huang
Sze Ter Lim
Ernult Franck Gerard
author_sort James Lourembam
title Role of CoFeB thickness in electric field controlled sub-100 nm sized magnetic tunnel junctions
title_short Role of CoFeB thickness in electric field controlled sub-100 nm sized magnetic tunnel junctions
title_full Role of CoFeB thickness in electric field controlled sub-100 nm sized magnetic tunnel junctions
title_fullStr Role of CoFeB thickness in electric field controlled sub-100 nm sized magnetic tunnel junctions
title_full_unstemmed Role of CoFeB thickness in electric field controlled sub-100 nm sized magnetic tunnel junctions
title_sort role of cofeb thickness in electric field controlled sub-100 nm sized magnetic tunnel junctions
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2018-05-01
description We report a comprehensive study on the role of the free layer thickness (tF) in electric-field controlled nanoscale perpendicular magnetic tunnel junctions (MTJs), comprising of free layer structure Ta/Co40Fe40B20/MgO, by using dc magnetoresistance and ultra-short magnetization switching measurements. Focusing on MTJs that exhibits positive effective device anisotropy (Keff), we observe that both the voltage-controlled magnetic anisotropy (ξ) and voltage modulation of coercivity show strong dependence on tF. We found that ξ varies dramatically and unexpectedly from ∼−3 fJ/V-m to ∼−41 fJ/V-m with increasing tF. We discuss the possibilities of electric-field tuning of the effective surface anisotropy term, KS as well as an additional interfacial magnetoelastic anisotropy term, K3 that scales with 1/tF2. Voltage pulse induced 180° magnetization reversal is also demonstrated in our MTJs. Unipolar switching and oscillatory function of switching probability vs. pulse duration can be observed at higher tF, and agrees well with the two key device parameters — Keff and ξ.
url http://dx.doi.org/10.1063/1.5006368
work_keys_str_mv AT jameslourembam roleofcofebthicknessinelectricfieldcontrolledsub100nmsizedmagnetictunneljunctions
AT jianchenghuang roleofcofebthicknessinelectricfieldcontrolledsub100nmsizedmagnetictunneljunctions
AT szeterlim roleofcofebthicknessinelectricfieldcontrolledsub100nmsizedmagnetictunneljunctions
AT ernultfranckgerard roleofcofebthicknessinelectricfieldcontrolledsub100nmsizedmagnetictunneljunctions
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