2019
DOI: 10.1016/j.actamat.2019.09.051
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Non-synchronized rotation of layered spin configurations in La0.825Sr0.175MnO3 /SrTiO3 film

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Cited by 3 publications
(1 citation statement)
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“…Strikingly, a fluctuation near the coercive field is collected at 10 K, which has never been observed before in the NCO system ( R xy – H ⊥ of the single-phase metallic NCO film is shown in Figure S4c). Commonly, the topological Hall effect at low fields and low temperatures appears in magnetic materials with the Dzyaloshinskii–Moriya interaction (DMI) due to the broken inversion symmetry and strong spin–orbital coupling at the interface. The band structure of NCO is very complex with no evidence of the topological feature, so the topological Hall effect can be excluded. The anomalous Hall resistance jump happens near the coercive field where a significant magnetic domain varies.…”
Section: Resultssupporting
confidence: 67%
“…Strikingly, a fluctuation near the coercive field is collected at 10 K, which has never been observed before in the NCO system ( R xy – H ⊥ of the single-phase metallic NCO film is shown in Figure S4c). Commonly, the topological Hall effect at low fields and low temperatures appears in magnetic materials with the Dzyaloshinskii–Moriya interaction (DMI) due to the broken inversion symmetry and strong spin–orbital coupling at the interface. The band structure of NCO is very complex with no evidence of the topological feature, so the topological Hall effect can be excluded. The anomalous Hall resistance jump happens near the coercive field where a significant magnetic domain varies.…”
Section: Resultssupporting
confidence: 67%