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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...
Autores principales: | , , , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group
2014
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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 |
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. |
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