Strain-induced perpendicular magnetic anisotropy in La$_2$CoMnO$_{6-\epsilon}$ thin films and its dependence with film thickness
Phys. Rev. B 93, 144417 (2016) Ferromagnetic insulating La$_2$CoMnO$_{6-\epsilon}$ (LCMO) epitaxial thin films grown on top of SrTiO$_3$ (001) substrates presents a strong magnetic anisotropy favoring the out of plane orientation of the magnetization with a strong anisotropy field ($\sim 70$ kOe for...
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Main Authors | , , , , , , , |
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Format | Journal Article |
Language | English |
Published |
29.10.2015
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Subjects | |
Online Access | Get full text |
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Summary: | Phys. Rev. B 93, 144417 (2016) Ferromagnetic insulating La$_2$CoMnO$_{6-\epsilon}$ (LCMO) epitaxial thin
films grown on top of SrTiO$_3$ (001) substrates presents a strong magnetic
anisotropy favoring the out of plane orientation of the magnetization with a
strong anisotropy field ($\sim 70$ kOe for film thickness of about 15 nm) and
with a coercive field of about 10 kOe. The anisotropy can be tuned by modifying
the oxygen content of the film which indirectly has two effects on the unit
cell: i) change of the orientation of the LCMO crystallographic axis over the
substrate (from c in-plane to c out-of-plane) and ii) shrinkage of the out of
plane cell parameter, which implies increasing tensile strain of the films. In
contrast, LCMO films grown on (LaAlO$_3$)$_{0.3}$(Sr$_2$AlTaO$_6$)$_{0.7}$ and
LaAlO$_3$ substrates (with a larger out-of-plane lattice parameter and
compressive stress) display in-plane magnetic anisotropy. Thus, we link the
strong magnetic anisotropy observed in La$_2$CoMnO$_{6-\epsilon}$ to the
relation between in-plane and out-of-plane parameters and so to the film
stress. |
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DOI: | 10.48550/arxiv.1510.08685 |