Deformation of spin-hedgehog lattice in MnGe
ORAL
Abstract
In a chiral magnet MnGe, there appears a spin hedgehog crystal, which is a lattice of spin hedgehogs and antihedgehogs formed from a superposition of three orthogonal helical spin structures [1]. The three-dimensional topological spin arrangements of hedgehogs and antihedgehogs serve as quantized sources and sinks of emergent magnetic fields, i.e., emergent magnetic monopoles, resulting in unconventional transport properties [2].
We observe a dramatic change in the Hall effect upon the transformation of a spin hedgehog crystal in MnGe through combined measurements of magnetotransport in single crystals and small-angle neutron scattering (SANS) [3]. At low temperatures, well-defined SANS peaks and a negative Hall signal are each consistent with expectations for a static hedgehog lattice. In contrast, a positive Hall signal takes over when the hedgehog lattice fluctuates at higher temperatures, with a diffuse SANS signal observed upon decomposition of the hedgehog lattice.
This result is indispensable for understanding the dynamics of emergent monopoles and gives a clue to their manipulation.
[1] N. Kanazawa et al., Nat. Commun. 7, 11622 (2016). [2] Y. Fujishiro et al., Nat. Commun. 9, 408 (2018). [3] N. Kanazawa, A. Kitaori, J. S. White et al., Phys. Rev. Lett. 125, 137202 (2020).
We observe a dramatic change in the Hall effect upon the transformation of a spin hedgehog crystal in MnGe through combined measurements of magnetotransport in single crystals and small-angle neutron scattering (SANS) [3]. At low temperatures, well-defined SANS peaks and a negative Hall signal are each consistent with expectations for a static hedgehog lattice. In contrast, a positive Hall signal takes over when the hedgehog lattice fluctuates at higher temperatures, with a diffuse SANS signal observed upon decomposition of the hedgehog lattice.
This result is indispensable for understanding the dynamics of emergent monopoles and gives a clue to their manipulation.
[1] N. Kanazawa et al., Nat. Commun. 7, 11622 (2016). [2] Y. Fujishiro et al., Nat. Commun. 9, 408 (2018). [3] N. Kanazawa, A. Kitaori, J. S. White et al., Phys. Rev. Lett. 125, 137202 (2020).
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Presenters
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Aki Kitaori
Univ of Tokyo
Authors
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Aki Kitaori
Univ of Tokyo
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Naoya Kanazawa
Univ of Tokyo
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Jonathan S White
Paul Scherrer Institute
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Victor Ukleev
Paul Scherrer Institute
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Henrik M Ronnow
Ecole Polytechnique Federale de Lausanne, École Polytechnique Fédérale de Lausanne (EPFL)
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Atsushi Tsukazaki
Tohoku University, Tohoku Univ.
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Masakazu Ichikawa
Univ of Tokyo
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Masashi Kawasaki
University of Tokyo, RIKEN, Univ of Tokyo, the University of Tokyo, Applied Physics and Quantum-Phase Electronics Center,, University of Tokyo
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Yoshinori Tokura
RIKEN, RIKEN Center for Emergent Matter Science and Tokyo College, The University of Tokyo, CEMS, RIKEN, RIKEN CEMS, Univ of Tokyo, Department of Applied Physics, The University of Tokyo