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Absence of zero-field-cooled exchange bias effect in single crystalline La2xAx CoMnO6 (A=Ca,Sr) compounds

C. Macchiutti, J. R. Jesus, F. B. Carneiro, L. Bufaiçal, M. Ciomaga Hatnean, G. Balakrishnan, and E. M. Bittar
Phys. Rev. Materials 5, 094402 – Published 7 September 2021

Abstract

Magnetic properties of A2BBO6 (A=rare or alkaline-earth ions; B,B=transitionmetal ions) double perovskites are of great interest due to their potential spintronic applications. Particularly fascinating is the zero-field-cooled exchange bias effect observed for the hole-doped La2xAxCoMnO6 polycrystalline samples. In this paper we synthesize La2CoMnO6,La1.5Ca0.5CoMnO6, and La1.5Sr0.5CoMnO6 single crystals by the floating zone method and study their magnetic behavior. The three materials are ferromagnetic. Surprisingly, we observe no zero or even conventional exchange bias effect for the Ca- and Sr-doped single crystals, in sharp contrast to polycrystalline samples. This absence indicates that the lack of grain boundaries and spin-glass-like behavior, not observed in our samples, might be key ingredients for the spontaneous exchange bias phenomena seen in polycrystalline samples.

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  • Received 25 May 2021
  • Accepted 26 August 2021

DOI:https://doi.org/10.1103/PhysRevMaterials.5.094402

©2021 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

C. Macchiutti1, J. R. Jesus1, F. B. Carneiro1, L. Bufaiçal2, M. Ciomaga Hatnean3, G. Balakrishnan3, and E. M. Bittar1,*

  • 1Centro Brasileiro de Pesquisas Físicas, Rio de Janeiro, Rio de Janeiro 22290-180, Brazil
  • 2Instituto de Física, Universidade Federal de Goiás, Goiânia 74001-970, Brazil
  • 3Department of Physics, University of Warwick, Coventry CV4 7AL, United Kingdom

  • *bittar@cbpf.br

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Vol. 5, Iss. 9 — September 2021

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Images

  • Figure 1
    Figure 1

    Conventional CuKα x-ray powder-diffraction patterns for (a) LCMO, (b) LCCMO, and (c) LSCMO. Open black circles are experimental data; red curves calculated Rietveld refinement; blue curves are the difference between the observed and the calculated patterns.

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  • Figure 2
    Figure 2

    X-ray Laue backreflection photograph, showing the [001] orientation of an aligned sample piece used for physical property measurements for (a) LCMO, (b) LCCMO, and (c) LSCMO. (d) LCCMO as-grown single crystal boule grown by the floating zone method.

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  • Figure 3
    Figure 3

    LCMO, LCCMO, and LSCMO as-grown single crystals temperature dependence of the ZFC and FC magnetization curves for H[001], measured at H=0.1kOe. The inset: Zero-magnetic-field heat capacity as a function of temperature.

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  • Figure 4
    Figure 4

    LCMO, LCCMO, and LSCMO single crystals in-phase component of ZFC ac susceptibility (χ) as a function of temperature for different frequencies in a probing ac magnetic field of 5 Oe.

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  • Figure 5
    Figure 5

    LCMO, LCCMO, and LSCMO ZFC as-grown single crystals M(H) curves for H[001], measured at T=5K and Hmax=90kOe. The right inset shows the magnified view of the curves close to the M=0 region. The left inset shows the LCCMO M(H) curve.

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