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Giant electrical modulation of magnetization in Co(40)Fe(40)B(20)/Pb(Mg(1/3)Nb(2/3))(0.7)Ti(0.3)O(3)(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 (ΔM/M) up to 83% with a 90° rotation of the easy axis...

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Detalles Bibliográficos
Autores principales: Zhang, Sen, Zhao, Yonggang, Xiao, Xia, Wu, Yizheng, Rizwan, Syed, Yang, Lifeng, Li, Peisen, Wang, Jiawei, Zhu, Meihong, Zhang, Huiyun, Jin, Xiaofeng, Han, Xiufeng
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2014
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3893657/
https://www.ncbi.nlm.nih.gov/pubmed/24430913
http://dx.doi.org/10.1038/srep03727
Descripción
Sumario: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 (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.