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Helical magnetic structure and the anomalous and topological Hall effects in epitaxial B20 Fe1yCoyGe films

Charles S. Spencer, Jacob Gayles, Nicholas A. Porter, Satoshi Sugimoto, Zabeada Aslam, Christian J. Kinane, Timothy R. Charlton, Frank Freimuth, Stanislav Chadov, Sean Langridge, Jairo Sinova, Claudia Felser, Stefan Blügel, Yuriy Mokrousov, and Christopher H. Marrows
Phys. Rev. B 97, 214406 – Published 6 June 2018

Abstract

Epitaxial films of the B20-structure compound Fe1yCoyGe were grown by molecular beam epitaxy on Si (111) substrates. The magnetization varied smoothly from the bulklike values of one Bohr magneton per Fe atom for FeGe to zero for nonmagnetic CoGe. The chiral lattice structure leads to a Dzyaloshinskii-Moriya interaction (DMI), and the films' helical magnetic ground state was confirmed using polarized neutron reflectometry measurements. The pitch of the spin helix, measured by this method, varies with Co content y and diverges at y0.45. This indicates a zero crossing of the DMI, which we reproduced in calculations using first-principles methods. We also measured the longitudinal and Hall resistivity of our films as a function of magnetic field, temperature, and Co content y. The Hall resistivity is expected to contain contributions from the ordinary, anomalous, and topological Hall effects. Both the anomalous and topological Hall resistivities show peaks around y0.5. Our first-principles calculations show a peak in the topological Hall constant at this value of y, related to the strong spin polarization predicted for intermediate values of y. Our calculations predict half-metallicity for y=0.6, consistent with the experimentally observed linear magnetoresistance at this composition, and potentially related to the other unusual transport properties for intermediate value of y. While it is possible to reconcile theory with experiment for the various Hall effects for FeGe, the large topological Hall resistivities for y0.5 are much larger than expected when the very small emergent fields associated with the divergence in the DMI are taken into account.

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  • Received 12 March 2018
  • Revised 4 May 2018
  • Corrected 25 June 2018

DOI:https://doi.org/10.1103/PhysRevB.97.214406

©2018 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Corrections

25 June 2018

Correction: The URL for the data repository contained an error and has been fixed.

Authors & Affiliations

Charles S. Spencer1, Jacob Gayles2,3, Nicholas A. Porter1, Satoshi Sugimoto1,*, Zabeada Aslam4, Christian J. Kinane5, Timothy R. Charlton5,†, Frank Freimuth6, Stanislav Chadov2, Sean Langridge5, Jairo Sinova3,7, Claudia Felser2, Stefan Blügel6, Yuriy Mokrousov3,6, and Christopher H. Marrows1

  • 1School of Physics and Astronomy, University of Leeds, Leeds LS2 9JT, United Kingdom
  • 2Max Planck Institute for Chemical Physics of Solids, 01187 Dresden, Germany
  • 3Institut für Physik, Johannes Gutenberg Universität Mainz, D-55099 Mainz, Germany
  • 4Leeds Electron Microscopy and Spectroscopy Centre, School of Chemical and Process Engineering, University of Leeds, Leeds LS2 9JT, United Kingdom
  • 5ISIS Neutron and Muon Source, STFC Rutherford Appleton Laboratory, Chilton, Didcot, Oxon OX11 0QX, United Kingdom
  • 6Peter Grünberg Institut & Institute for Advanced Simulation, Forschungszentrum Jülich and JARA, 52425 Jülich, Germany
  • 7Institute of Physics ASCR, v.v.i., Cukrovarnicka 10, 162 53 Praha 6, Czech Republic

  • *Present address: Institute for Solid State Physics, University of Tokyo, 5-1-5 Kashiwa-no-ha, Kashiwa, Chiba 277-8581, Japan.
  • Present address: Neutron Scattering Division, P.O. Box 2008 MS 6473, Oak Ridge National Lab, Oak Ridge, TN 37831-6473.

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Issue

Vol. 97, Iss. 21 — 1 June 2018

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