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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2018-05-01
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Online Access: | http://dx.doi.org/10.1063/1.5006368 |
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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 |
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