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Switching of a large anomalous Hall effect between metamagnetic phases of a non-collinear antiferromagnet.


ABSTRACT: The anomalous Hall effect (AHE), which in long-range ordered ferromagnets appears as a voltage transverse to the current and usually is proportional to the magnetization, often is believed to be of negligible size in antiferromagnets due to their low uniform magnetization. However, recent experiments and theory have demonstrated that certain antiferromagnets with a non-collinear arrangement of magnetic moments exhibit a sizeable spontaneous AHE at zero field due to a non-vanishing Berry curvature arising from the quantum mechanical phase of the electron's wave functions. Here we show that antiferromagnetic Mn5Si3 single crystals exibit a large AHE which is strongly anisotropic and shows multiple transitions with sign changes at different magnetic fields due to field-induced rearrangements of the magnetic structure despite only tiny variations of the total magnetization. The presence of multiple non-collinear magnetic phases offers the unique possiblity to explore the details of the AHE and the sensitivity of the Hall effect on the details of the magnetic texture.

SUBMITTER: Surgers C 

PROVIDER: S-EPMC5317170 | biostudies-literature | 2017 Feb

REPOSITORIES: biostudies-literature

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Switching of a large anomalous Hall effect between metamagnetic phases of a non-collinear antiferromagnet.

Sürgers Christoph C   Wolf Thomas T   Adelmann Peter P   Kittler Wolfram W   Fischer Gerda G   Löhneysen Hilbert V HV  

Scientific reports 20170220


The anomalous Hall effect (AHE), which in long-range ordered ferromagnets appears as a voltage transverse to the current and usually is proportional to the magnetization, often is believed to be of negligible size in antiferromagnets due to their low uniform magnetization. However, recent experiments and theory have demonstrated that certain antiferromagnets with a non-collinear arrangement of magnetic moments exhibit a sizeable spontaneous AHE at zero field due to a non-vanishing Berry curvatur  ...[more]

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