Complex strain evolution of polar and magnetic order in multiferroic BiFeO3 thin films

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作者
Zuhuang Chen
Zhanghui Chen
Chang-Yang Kuo
Yunlong Tang
Liv R. Dedon
Qian Li
Lei Zhang
Christoph Klewe
Yen-Lin Huang
Bhagwati Prasad
Alan Farhan
Mengmeng Yang
James D. Clarkson
Sujit Das
Sasikanth Manipatruni
A. Tanaka
Padraic Shafer
Elke Arenholz
Andreas Scholl
Ying-Hao Chu
Z. Q. Qiu
Zhiwei Hu
Liu-Hao Tjeng
Ramamoorthy Ramesh
Lin-Wang Wang
Lane W. Martin
机构
[1] Harbin Institute of Technology,School of Materials Science and Engineering
[2] University of California,Department of Materials Science and Engineering
[3] Lawrence Berkeley National Laboratory,Materials Sciences Division
[4] Max-Planck Institute for Chemical Physics of Solids,Department of Physics
[5] National Synchrotron Radiation Research Center,Advanced Light Source
[6] University of California,Components Research
[7] Lawrence Berkeley National Laboratory,Department of Quantum Matter, ADSM
[8] Intel Corp.,Department of Materials Science and Engineering
[9] Hiroshima University,undefined
[10] National Chiao Tung University,undefined
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摘要
Electric-field control of magnetism requires deterministic control of the magnetic order and understanding of the magnetoelectric coupling in multiferroics like BiFeO3 and EuTiO3. Despite this critical need, there are few studies on the strain evolution of magnetic order in BiFeO3 films. Here, in (110)-oriented BiFeO3 films, we reveal that while the polarization structure remains relatively unaffected, strain can continuously tune the orientation of the antiferromagnetic-spin axis across a wide angular space, resulting in an unexpected deviation of the classical perpendicular relationship between the antiferromagnetic axis and the polarization. Calculations suggest that this evolution arises from a competition between the Dzyaloshinskii–Moriya interaction and single-ion anisotropy wherein the former dominates at small strains and the two are comparable at large strains. Finally, strong coupling between the BiFeO3 and the ferromagnet Co0.9Fe0.1 exists such that the magnetic anisotropy of the ferromagnet can be effectively controlled by engineering the orientation of the antiferromagnetic-spin axis.
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