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Giant doping response of magnetic anisotropy in MnTe

Duncan H. Moseley, Keith M. Taddei, Jiaqiang Yan, Michael A. McGuire, Stuart Calder, M. M. H. Polash, Daryoosh Vashaee, Xiaofan Zhang, Huaizhou Zhao, David S. Parker, Randy S. Fishman, and Raphaël P. Hermann
Phys. Rev. Materials 6, 014404 – Published 18 January 2022
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Abstract

Developing simple ways to control spin states in spintronic devices is a crucial step towards increasing their functionality. MnTe is a room-temperature antiferromagnet with promising spintronic properties, including for thermospintronics and magnon-based devices. Here, we show that, in MnTe, less than 1% Li is sufficient to produce a dramatic spin reorientation as observed by neutron diffraction. The behavior of the 0001 magnetic Bragg peak reveals a significant reorientation of the Mn spins from planar in the pure material to almost completely axial with minimal Li doping. Temperature dependence of the magnetic peaks in Li-doped samples indicates that axial spins shift back to planar suddenly upon approaching the Néel temperature (TN=307 K). Density functional theory calculations support the idea that a shift in the Fermi level caused by doping is responsible for switching the material between two competing magnetic ground states. These results pave the way for developing easy switching of magnetic states in functional materials such as spintronic devices and topological insulators.

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  • Received 17 March 2021
  • Accepted 6 December 2021

DOI:https://doi.org/10.1103/PhysRevMaterials.6.014404

©2022 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Duncan H. Moseley1, Keith M. Taddei2, Jiaqiang Yan1, Michael A. McGuire1, Stuart Calder2, M. M. H. Polash3,4, Daryoosh Vashaee3,4, Xiaofan Zhang5, Huaizhou Zhao5, David S. Parker1, Randy S. Fishman1, and Raphaël P. Hermann1,*

  • 1Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 2Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 3Department of Electrical and Computer Engineering, North Carolina State University, Raleigh, North Carolina 27606, USA
  • 4Department of Materials Science and Engineering, North Carolina State University, Raleigh, North Carolina 27606, USA
  • 5Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China

  • *hermannrp@ornl.gov

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Issue

Vol. 6, Iss. 1 — January 2022

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