Coexistence of magnetic order and spin-glass-like phase in the pyrochlore antiferromagnet Na3Co(CO3)2Cl

Zhendong Fu, Yanzhen Zheng, Yinguo Xiao, Subhankar Bedanta, Anatoliy Senyshyn, Giovanna Giulia Simeoni, Yixi Su, Ulrich Rücker, Paul Kögerler, and Thomas Brückel
Phys. Rev. B 87, 214406 – Published 6 June 2013

Abstract

We present comprehensive investigations on a pyrochlore antiferromagnet Na3Co(CO3)2Cl. Performed dc magnetization indicates a broad maximum at around 4 K. The field dependence of the peak temperature of this maximum follows the de Almeida–Thouless line, suggesting a spin-glass-like phase transition. The ac susceptibility measurements determine the glassy transition temperature to be 4.5 K and reveal a frequency-independent peak at 17 K. The temperature dependence of the specific heat shows a sharp peak at 1.5 K and a broad hump at around 5 K, which are attributed to a long-range magnetic phase transition and a spin-glass-like freezing process, respectively. The average crystallographic structure of Na3Co(CO3)2Cl has been determined using neutron-powder diffraction. No obvious site disorder has been detected within the experimental resolution. The diffuse neutron scattering with polarization analysis indicates short-range spin correlations characterized by dominating antiferromagnetic coupling between nearest neighbors and weak ferromagnetic coupling between next-nearest neighbors. The long-range magnetic order below 1.5 K is evidenced by the magnetic reflections observed at 50 mK and can be well explained with an all-in–all-out spin configuration. Inelastic neutron scattering of Na3Co(CO3)2Cl exhibits collective magnetic excitations at 3.5 K, suggesting that the spin-glass-like transition temperature Tg = 4.5 K does not correspond to a complete spin-glass freezing as expected in canonical spin glasses. The peak observed in magnetic susceptibility at 17 K is attributed to the onset of an intermediate partially ordered phase transition, qualitatively consistent with the theoretical predictions for pyrochlore antiferromagnets with weak ferromagnetic next-nearest-neighbor interactions.

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  • Received 20 January 2013

DOI:https://doi.org/10.1103/PhysRevB.87.214406

©2013 American Physical Society

Authors & Affiliations

Zhendong Fu1,*, Yanzhen Zheng2,7,†, Yinguo Xiao3, Subhankar Bedanta4, Anatoliy Senyshyn5,6, Giovanna Giulia Simeoni5, Yixi Su1, Ulrich Rücker3, Paul Kögerler3,7, and Thomas Brückel3,‡

  • 1Jülich Centre for Neutron Science JCNS, Forschungszentrum Jülich GmbH, Outstation at FRM II, Lichtenbergstraße 1, D-85747 Garching b. München, Germany
  • 2Center for Applied Chemical Research, Frontier Institute of Science and Technology, Xi'an Jiaotong University, 710049 Xi'an, China
  • 3Jülich Centre for Neutron Science JCNS, Peter Grünberg Institut PGI, JARA-FIT, Forschungszentrum Jülich GmbH, D-52425 Jülich, Germany
  • 4School of Physical Sciences, National Institute of Science Education and Research, 751005 Orissa, India
  • 5Forschungsneutronenquelle Heinz-Maier Leibnitz FRM II, Technische Universität München, Lichtenbergstraße 1, D-85747 Garching b. München, Germany
  • 6Institute for Material Science, Darmstadt University of Technology, D-64287 Darmstadt, Germany
  • 7Institut für Anorganische Chemie, RWTH Aachen University, D-52074 Aachen, Germany

  • *fuzhendong@gmail.com
  • zhengyanzhen@gmail.com
  • t.brueckel@fz-juelich.de

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Issue

Vol. 87, Iss. 21 — 1 June 2013

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