Composition dependence of the second-order interfacial magnetic anisotropy for MgO/CoFeB/Ta films
The CoFeB thickness, t dependence of the effective first- and second-order magnetic anisotropy, K1eff and K2, for MgO/(Co1-xFex)80B20/Ta films (x=0.3-1.0) is investigated. As Co40Fe40B20 thickness decreases, K1eff increases and shows a perpendicular magnetic anisotropy for t=1.2 nm. On the other han...
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doaj-a7df4b0a84a549fcafd79b6ced3b933c2020-11-25T02:15:56ZengAIP Publishing LLCAIP Advances2158-32262019-12-01912125053125053-510.1063/1.5129988Composition dependence of the second-order interfacial magnetic anisotropy for MgO/CoFeB/Ta filmsTakahiro Ogasawara0Mikihiko Oogane1Muftah Al-Mahdawi2Masakiyo Tsunoda3Yasuo Ando4Department of Applied Physics, Tohoku University, Sendai 980-8579, JapanDepartment of Applied Physics, Tohoku University, Sendai 980-8579, JapanCenter for Science and Innovation in Spintronics (Core Research Cluster) Organization for Advanced Studies, Tohoku University, Sendai 980-8577, JapanCenter for Spintronics Research Network, Tohoku University, Sendai 980-8577, JapanDepartment of Applied Physics, Tohoku University, Sendai 980-8579, JapanThe CoFeB thickness, t dependence of the effective first- and second-order magnetic anisotropy, K1eff and K2, for MgO/(Co1-xFex)80B20/Ta films (x=0.3-1.0) is investigated. As Co40Fe40B20 thickness decreases, K1eff increases and shows a perpendicular magnetic anisotropy for t=1.2 nm. On the other hand, in-plane magnetic anisotropy is observed for t≥1.4 nm. Also, a 1.3-nm-thick CoFeB sample demonstrates an easy-cone behavior, which suggests that the magnitude of K1eff and K2 becomes comparable. By plotting the product of K2 and t-td as a function of t-td, where td is a magnetic dead layer thickness, linear dependences with negative y-axis intercepts are displayed for all ranges of x. The extracted interfacial K2, Ki(2) are varied depending on the compositions in the range of-0.024 to −0.042 erg/cm2 for x=100% and 30, 50%, respectively. A magnetic phase diagram summarizing the results of K1-2πMs2 and K2 suggests that the ratio of K2 against K1-2πMs2 is varied depending on the compositions. These results give us a guideline to achieve the desired magnetic properties of CoFeB for spintronic applications.http://dx.doi.org/10.1063/1.5129988 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Takahiro Ogasawara Mikihiko Oogane Muftah Al-Mahdawi Masakiyo Tsunoda Yasuo Ando |
spellingShingle |
Takahiro Ogasawara Mikihiko Oogane Muftah Al-Mahdawi Masakiyo Tsunoda Yasuo Ando Composition dependence of the second-order interfacial magnetic anisotropy for MgO/CoFeB/Ta films AIP Advances |
author_facet |
Takahiro Ogasawara Mikihiko Oogane Muftah Al-Mahdawi Masakiyo Tsunoda Yasuo Ando |
author_sort |
Takahiro Ogasawara |
title |
Composition dependence of the second-order interfacial magnetic anisotropy for MgO/CoFeB/Ta films |
title_short |
Composition dependence of the second-order interfacial magnetic anisotropy for MgO/CoFeB/Ta films |
title_full |
Composition dependence of the second-order interfacial magnetic anisotropy for MgO/CoFeB/Ta films |
title_fullStr |
Composition dependence of the second-order interfacial magnetic anisotropy for MgO/CoFeB/Ta films |
title_full_unstemmed |
Composition dependence of the second-order interfacial magnetic anisotropy for MgO/CoFeB/Ta films |
title_sort |
composition dependence of the second-order interfacial magnetic anisotropy for mgo/cofeb/ta films |
publisher |
AIP Publishing LLC |
series |
AIP Advances |
issn |
2158-3226 |
publishDate |
2019-12-01 |
description |
The CoFeB thickness, t dependence of the effective first- and second-order magnetic anisotropy, K1eff and K2, for MgO/(Co1-xFex)80B20/Ta films (x=0.3-1.0) is investigated. As Co40Fe40B20 thickness decreases, K1eff increases and shows a perpendicular magnetic anisotropy for t=1.2 nm. On the other hand, in-plane magnetic anisotropy is observed for t≥1.4 nm. Also, a 1.3-nm-thick CoFeB sample demonstrates an easy-cone behavior, which suggests that the magnitude of K1eff and K2 becomes comparable. By plotting the product of K2 and t-td as a function of t-td, where td is a magnetic dead layer thickness, linear dependences with negative y-axis intercepts are displayed for all ranges of x. The extracted interfacial K2, Ki(2) are varied depending on the compositions in the range of-0.024 to −0.042 erg/cm2 for x=100% and 30, 50%, respectively. A magnetic phase diagram summarizing the results of K1-2πMs2 and K2 suggests that the ratio of K2 against K1-2πMs2 is varied depending on the compositions. These results give us a guideline to achieve the desired magnetic properties of CoFeB for spintronic applications. |
url |
http://dx.doi.org/10.1063/1.5129988 |
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