Correlation between site occupancies and spin-glass transition in skyrmion host Co10x2Zn10x2Mnx

T. Nakajima, K. Karube, Y. Ishikawa, M. Yonemura, N. Reynolds, J. S. White, H. M. Rønnow, A. Kikkawa, Y. Tokunaga, Y. Taguchi, Y. Tokura, and T. Arima
Phys. Rev. B 100, 064407 – Published 16 August 2019

Abstract

Ternary alloys Co-Zn-Mn with β-Mn-type structure exhibit helimagnetic order and skyrmion lattice states in a low-Mn-concentration region. Recent studies on Co10x2Zn10x2Mnx (CZM) revealed that the magnetic modulation period and the paramagnetic-to-helimagnetic transition temperature are reduced with increasing Mn concentration x [Tokunaga et al., Nat. Commun. 6, 7638 (2015)] and that the helimagnetic order is replaced with a spin-glass state in a high-x region [Karube et al., Sci. Adv. 4, eaar7043 (2018)]. To understand the microscopic mechanism of the Mn substitution effect, we have performed crystal structure analyses of a series of CZM samples with x=4,5,6,7,8,10,12, and 16 by neutron powder diffraction. We present a model for the site occupancies of Co, Zn, and Mn in the unit cell, which has two independent crystallographic sites, specifically 8c and 12d sites. Zn atoms are always accommodated in the 12d sites, and Co atoms prefer the 8c sites, although some of them also exist in the 12d sites in a low-x region. Mn atoms mainly prefer the 12d sites but also share the 8c site with Co atoms in the region of x4. A comparison between the site occupancies and the xT magnetic phase diagram suggests that the amount of Mn in the 8c sites is relevant to the emergence of the spin-glass state.

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  • Received 15 May 2019

DOI:https://doi.org/10.1103/PhysRevB.100.064407

©2019 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

T. Nakajima1,2,*, K. Karube2, Y. Ishikawa3, M. Yonemura3, N. Reynolds4,5, J. S. White4, H. M. Rønnow5, A. Kikkawa2, Y. Tokunaga2,6, Y. Taguchi2, Y. Tokura1,2, and T. Arima2,6

  • 1Department of Applied Physics and Quantum Phase Electronics Center, University of Tokyo, Tokyo 113-8656, Japan
  • 2RIKEN Center for Emergent Matter Science, Saitama 351-0198, Japan
  • 3Institute of Materials Structure Science, KEK, Tokai, Ibaraki 319-1106, Japan
  • 4Laboratory for Neutron Scattering and Imaging, Paul Scherrer Institute, CH-5232 Villigen, Switzerland
  • 5Laboratory for Quantum Magnetism, Institute of Physics, École Polytechnique Fédérale de Lausanne, CH-1015 Lausanne, Switzerland
  • 6Department of Advanced Materials Science, University of Tokyo, Kashiwa 277-8561, Japan

  • *taro.nakajima@ap.t.u-tokyo.ac.jp

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Vol. 100, Iss. 6 — 1 August 2019

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