Giant electrical modulation of magnetization in Co40Fe40B20/Pb(Mg1/3Nb2/3)0.7Ti0.3O3(011) heterostructure
We report a giant electric-field control of magnetization ( M ) as well as magnetic anisotropy in a Co 40 Fe 40 B 20 (CoFeB)/Pb(Mg 1/3 Nb 2/3 ) 0.7 Ti 0.3 O 3 (PMN-PT) structure at room temperature, in which a maximum relative magnetization change (Δ M / M ) up to 83% with a 90° rotation of the easy...
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| Published in | Scientific reports Vol. 4; no. 1; p. 3727 |
|---|---|
| Main Authors | , , , , , , , , , , , |
| Format | Journal Article |
| Language | English |
| Published |
London
Nature Publishing Group UK
16.01.2014
Nature Publishing Group |
| Subjects | |
| Online Access | Get full text |
| ISSN | 2045-2322 2045-2322 |
| DOI | 10.1038/srep03727 |
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| Abstract | We report a giant electric-field control of magnetization (
M
) as well as magnetic anisotropy in a Co
40
Fe
40
B
20
(CoFeB)/Pb(Mg
1/3
Nb
2/3
)
0.7
Ti
0.3
O
3
(PMN-PT) structure at room temperature, in which a maximum relative magnetization change (Δ
M
/
M
) up to 83% with a 90° rotation of the easy axis under electric fields were observed by different magnetic measurement systems with
in-situ
electric fields. The mechanism for this giant magnetoelectric (ME) coupling can be understood as the combination of the ultra-high value of anisotropic in-plane piezoelectric coefficients of (011)-cut PMN-PT due to ferroelectric polarization reorientation and the perfect soft ferromagnetism without magnetocrystalline anisotropy of CoFeB film. Besides the giant electric-field control of magnetization and magnetic anisotropy, this work has also demonstrated the feasibility of reversible and deterministic magnetization reversal controlled by pulsed electric fields with the assistance of a weak magnetic field, which is important for realizing strain-mediated magnetoelectric random access memories. |
|---|---|
| AbstractList | We report a giant electric-field control of magnetization (
M
) as well as magnetic anisotropy in a Co
40
Fe
40
B
20
(CoFeB)/Pb(Mg
1/3
Nb
2/3
)
0.7
Ti
0.3
O
3
(PMN-PT) structure at room temperature, in which a maximum relative magnetization change (Δ
M
/
M
) up to 83% with a 90° rotation of the easy axis under electric fields were observed by different magnetic measurement systems with
in-situ
electric fields. The mechanism for this giant magnetoelectric (ME) coupling can be understood as the combination of the ultra-high value of anisotropic in-plane piezoelectric coefficients of (011)-cut PMN-PT due to ferroelectric polarization reorientation and the perfect soft ferromagnetism without magnetocrystalline anisotropy of CoFeB film. Besides the giant electric-field control of magnetization and magnetic anisotropy, this work has also demonstrated the feasibility of reversible and deterministic magnetization reversal controlled by pulsed electric fields with the assistance of a weak magnetic field, which is important for realizing strain-mediated magnetoelectric random access memories. We report a giant electric-field control of magnetization (M) as well as magnetic anisotropy in a Co40 Fe40 B20 (CoFeB)/Pb(Mg1/3 Nb2/3 )0.7 Ti0.3 O3 (PMN-PT) structure at room temperature, in which a maximum relative magnetization change (ΔM/M) up to 83% with a 90° rotation of the easy axis under electric fields were observed by different magnetic measurement systems with in-situ electric fields. The mechanism for this giant magnetoelectric (ME) coupling can be understood as the combination of the ultra-high value of anisotropic in-plane piezoelectric coefficients of (011)-cut PMN-PT due to ferroelectric polarization reorientation and the perfect soft ferromagnetism without magnetocrystalline anisotropy of CoFeB film. Besides the giant electric-field control of magnetization and magnetic anisotropy, this work has also demonstrated the feasibility of reversible and deterministic magnetization reversal controlled by pulsed electric fields with the assistance of a weak magnetic field, which is important for realizing strain-mediated magnetoelectric random access memories. We report a giant electric-field control of magnetization (M) as well as magnetic anisotropy in a Co40Fe40B20(CoFeB)/Pb(Mg1/3Nb2/3)0.7Ti0.3O3(PMN-PT) structure at room temperature, in which a maximum relative magnetization change (ΔM/M) up to 83% with a 90° rotation of the easy axis under electric fields were observed by different magnetic measurement systems with in-situ electric fields. The mechanism for this giant magnetoelectric (ME) coupling can be understood as the combination of the ultra-high value of anisotropic in-plane piezoelectric coefficients of (011)-cut PMN-PT due to ferroelectric polarization reorientation and the perfect soft ferromagnetism without magnetocrystalline anisotropy of CoFeB film. Besides the giant electric-field control of magnetization and magnetic anisotropy, this work has also demonstrated the feasibility of reversible and deterministic magnetization reversal controlled by pulsed electric fields with the assistance of a weak magnetic field, which is important for realizing strain-mediated magnetoelectric random access memories. We report a giant electric-field control of magnetization (M) as well as magnetic anisotropy in a Co40Fe40B20(CoFeB)/Pb(Mg1/3Nb2/3)0.7Ti0.3O3(PMN-PT) structure at room temperature, in which a maximum relative magnetization change (ΔM/M) up to 83% with a 90° rotation of the easy axis under electric fields were observed by different magnetic measurement systems with in-situ electric fields. The mechanism for this giant magnetoelectric (ME) coupling can be understood as the combination of the ultra-high value of anisotropic in-plane piezoelectric coefficients of (011)-cut PMN-PT due to ferroelectric polarization reorientation and the perfect soft ferromagnetism without magnetocrystalline anisotropy of CoFeB film. Besides the giant electric-field control of magnetization and magnetic anisotropy, this work has also demonstrated the feasibility of reversible and deterministic magnetization reversal controlled by pulsed electric fields with the assistance of a weak magnetic field, which is important for realizing strain-mediated magnetoelectric random access memories.We report a giant electric-field control of magnetization (M) as well as magnetic anisotropy in a Co40Fe40B20(CoFeB)/Pb(Mg1/3Nb2/3)0.7Ti0.3O3(PMN-PT) structure at room temperature, in which a maximum relative magnetization change (ΔM/M) up to 83% with a 90° rotation of the easy axis under electric fields were observed by different magnetic measurement systems with in-situ electric fields. The mechanism for this giant magnetoelectric (ME) coupling can be understood as the combination of the ultra-high value of anisotropic in-plane piezoelectric coefficients of (011)-cut PMN-PT due to ferroelectric polarization reorientation and the perfect soft ferromagnetism without magnetocrystalline anisotropy of CoFeB film. Besides the giant electric-field control of magnetization and magnetic anisotropy, this work has also demonstrated the feasibility of reversible and deterministic magnetization reversal controlled by pulsed electric fields with the assistance of a weak magnetic field, which is important for realizing strain-mediated magnetoelectric random access memories. |
| ArticleNumber | 3727 |
| Author | Zhang, Sen Zhang, Huiyun Han, Xiufeng Zhao, Yonggang Wang, Jiawei Li, Peisen Rizwan, Syed Jin, Xiaofeng Xiao, Xia Yang, Lifeng Zhu, Meihong Wu, Yizheng |
| Author_xml | – sequence: 1 givenname: Sen surname: Zhang fullname: Zhang, Sen organization: Department of Physics and State Key Laboratory of Low-Dimensional Quantum Physics, Tsinghua University, College of Science, National University of Defense Technology – sequence: 2 givenname: Yonggang surname: Zhao fullname: Zhao, Yonggang organization: Department of Physics and State Key Laboratory of Low-Dimensional Quantum Physics, Tsinghua University, Collaborative Innovation Center of Quantum Matter – sequence: 3 givenname: Xia surname: Xiao fullname: Xiao, Xia organization: Department of Physics, State Key Laboratory of Surface Physics and Advanced Materials Laboratory, Fudan University – sequence: 4 givenname: Yizheng surname: Wu fullname: Wu, Yizheng organization: Department of Physics, State Key Laboratory of Surface Physics and Advanced Materials Laboratory, Fudan University – sequence: 5 givenname: Syed surname: Rizwan fullname: Rizwan, Syed organization: Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences – sequence: 6 givenname: Lifeng surname: Yang fullname: Yang, Lifeng organization: Department of Physics and State Key Laboratory of Low-Dimensional Quantum Physics, Tsinghua University – sequence: 7 givenname: Peisen surname: Li fullname: Li, Peisen organization: Department of Physics and State Key Laboratory of Low-Dimensional Quantum Physics, Tsinghua University – sequence: 8 givenname: Jiawei surname: Wang fullname: Wang, Jiawei organization: Department of Physics and State Key Laboratory of Low-Dimensional Quantum Physics, Tsinghua University – sequence: 9 givenname: Meihong surname: Zhu fullname: Zhu, Meihong organization: Department of Physics and State Key Laboratory of Low-Dimensional Quantum Physics, Tsinghua University – sequence: 10 givenname: Huiyun surname: Zhang fullname: Zhang, Huiyun organization: Department of Physics and State Key Laboratory of Low-Dimensional Quantum Physics, Tsinghua University – sequence: 11 givenname: Xiaofeng surname: Jin fullname: Jin, Xiaofeng organization: Department of Physics, State Key Laboratory of Surface Physics and Advanced Materials Laboratory, Fudan University – sequence: 12 givenname: Xiufeng surname: Han fullname: Han, Xiufeng organization: Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences |
| BackLink | https://www.ncbi.nlm.nih.gov/pubmed/24430913$$D View this record in MEDLINE/PubMed |
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| Copyright | The Author(s) 2014 Copyright Nature Publishing Group Jan 2014 Copyright © 2014, Macmillan Publishers Limited. All rights reserved 2014 Macmillan Publishers Limited. All rights reserved |
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| Snippet | We report a giant electric-field control of magnetization (
M
) as well as magnetic anisotropy in a Co
40
Fe
40
B
20
(CoFeB)/Pb(Mg
1/3
Nb
2/3
)
0.7
Ti
0.3
O
3... We report a giant electric-field control of magnetization (M) as well as magnetic anisotropy in a Co40Fe40B20(CoFeB)/Pb(Mg1/3Nb2/3)0.7Ti0.3O3(PMN-PT) structure... We report a giant electric-field control of magnetization (M) as well as magnetic anisotropy in a Co40 Fe40 B20 (CoFeB)/Pb(Mg1/3 Nb2/3 )0.7 Ti0.3 O3 (PMN-PT)... |
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| SubjectTerms | 639/301/119/996 639/301/119/997 Anisotropy Electric fields Humanities and Social Sciences Lead Magnetic fields multidisciplinary Polarization Science Temperature effects |
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| Title | Giant electrical modulation of magnetization in Co40Fe40B20/Pb(Mg1/3Nb2/3)0.7Ti0.3O3(011) heterostructure |
| URI | https://link.springer.com/article/10.1038/srep03727 https://www.ncbi.nlm.nih.gov/pubmed/24430913 https://www.proquest.com/docview/1897794676 https://www.proquest.com/docview/1490710049 https://pubmed.ncbi.nlm.nih.gov/PMC3893657 |
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