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Effect of structural and magnetic disorder on the 3d5d exchange interactions in La2xCaxCoIrO6

L. Bufaiçal, E. Sadrollahi, F. J. Litterst, D. Rigitano, E. Granado, L. T. Coutrim, E. B. Araújo, M. B. Fontes, E. Baggio-Saitovitch, and E. M. Bittar
Phys. Rev. B 102, 024436 – Published 22 July 2020
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Abstract

The delicate balance between spin-orbit coupling, Coulomb repulsion, and crystalline electric field interactions observed in Ir-based oxides is usually manifested as exotic magnetic behavior. Here we investigate the evolution of the exchange coupling between Co and Ir for partial La substitution by Ca in La2CoIrO6. A great advantage of the use of Ca2+ as a replacement for La3+ is the similarity of their ionic radii. Thus, the observed magnetic changes can more easily be associated with electronic variations. A thorough investigation of the structural, electronic, and magnetic properties of the La2xCaxCoIrO6 system was carried out by means of synchrotron x-ray powder diffraction, muon spin rotation and relaxation (μSR), AC and DC magnetization, x-ray absorption spectroscopy (XAS), x-ray magnetic circular dichroism, Raman spectroscopy, electrical resistivity, and dielectric permittivity. Our XAS results show that up to 25% Ca substitution at the La site results in the emergence of Co3+, possibly in a high-spin state, while the introduction of a larger amount of Ca leads to an increase in the Ir valence. The competing magnetic interactions resulting from the mixed valences lead to the coexistence of a magnetically ordered and an emerging spin-glass (SG) state for the doped samples. Our μSR results indicate that for La2CoIrO6 a nearly constant fraction of a paramagnetic (PM) phase persists down to low temperatures, possibly related to the presence of a small amount of Ir3+ and to the antisite disorder at Co/Ir sites. For doped compounds the PM phase freezes below 30 K, but there is still some dynamics associated with the SG. The dielectric data obtained for the parent compound and the one with 25% Ca doping indicate a possible magnetodielectric effect, which is discussed in terms of the electron hopping between the transition-metal ions, the antisite disorder at Co/Ir sites, and the distorted crystalline structure.

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  • Received 7 March 2020
  • Revised 1 June 2020
  • Accepted 8 July 2020

DOI:https://doi.org/10.1103/PhysRevB.102.024436

©2020 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

L. Bufaiçal1,*, E. Sadrollahi2,3, F. J. Litterst2,4,†, D. Rigitano5, E. Granado5, L. T. Coutrim1,6, E. B. Araújo7, M. B. Fontes4, E. Baggio-Saitovitch4, and E. M. Bittar4

  • 1Instituto de Física, Universidade Federal de Goiás, 74001-970 Goiânia, Goiás, Brazil
  • 2Institut für Physik der Kondensierten Materie, Technische Universität Braunschweig, 38106 Braunschweig, Germany
  • 3Institut für Festkörper- und Materialphysik, Technische Universität Dresden, 01069 Dresden, Germany
  • 4Centro Brasileiro de Pesquisas Físicas, 22290-180 Rio de Janeiro, Rio de Janeiro, Brazil
  • 5Instituto de Física “Gleb Wataghin,” UNICAMP, 13083-859 Campinas, São Paulo, Brazil
  • 6Laboratório Nacional de Luz Síncrotron, Centro Nacional de Pesquisa em Energia e Materiais, 13083-970 Campinas, São Paulo, Brazil
  • 7Department of Physics and Chemistry, São Paulo State University, 15385-000 Ilha Solteira, São Paulo, Brazil

  • *lbufaical@ufg.br
  • j.litterst@tu-braunschweig.de

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Issue

Vol. 102, Iss. 2 — 1 July 2020

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Images

  • Figure 1
    Figure 1

    Magnified view of the (020), (112), (112¯), and (200) Bragg reflections in the SXRD patterns of La2xCaxCoIrO6. Inset: a, b, and c lattice parameters as a function of the Ca concentration, x.

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  • Figure 2
    Figure 2

    (a) Co-K edge XAS spectra of La2xCaxCoIrO6 samples. The spectra of CoO and LaCoO3 are also displayed as references for Co2+ and Co3+, respectively. The presence of two white lines, indicating a Co2+/Co3+ mixed valence state, is highlighted by arrows on the curve of the x=0.5 sample. (b) Ir-L3 spectra, together with those of IrO2 and Sr2FeIrO6, reference samples for Ir4+ and Ir5+, respectively. Inset: Magnified view of the absorption edges.

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  • Figure 3
    Figure 3

    The 60 K Ir-L3 XANES spectrum for x=0 and XMCD spectra for x=0, 0.5, 0.8, and 1.0 samples.

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  • Figure 4
    Figure 4

    Raman spectra of the La2xCaxCoIrO6 samples at 23 K.

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  • Figure 5
    Figure 5

    (a) ZFC and FC M(T) curves for La2xCaxCoIrO6, measured at H=500 Oe. Inset: Magnified view of the ZFC curves, evidencing TC1, TC2, and Tf. (b) M(H) curves measured at T=5K. Inset: Magnified view of the x=0 curve near the H=0 region.

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  • Figure 6
    Figure 6

    χ as a function of T for (a) x=0.8 and (b) x=1.0 samples. Vertical lines are guidelines for TC1 and TC2 determined from the inflection points in the curves. Insets: Tf as a function of f, where solid lines represent the best fits to the data using Eq. (1).

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  • Figure 7
    Figure 7

    (a) μSR rotation patterns of La2CoIrO6 in a weak applied transverse field (wTF) of 50 Oe at some selected temperatures; (b) variation of a weakly damped PM fraction with temperature derived from wTF spectra.

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  • Figure 8
    Figure 8

    ZF μSR patterns of La2CoIrO6 at some selected temperatures for a time window of 0–0.2 μs, showing spontaneous muon spin rotation in the magnetically ordered state.

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  • Figure 9
    Figure 9

    DC electrical resistivity (ρ) as a function of the temperature for La2xCaxCoIrO6 samples. Solid lines represent the best fit of the data with Eq. (6). Inset: Evolution of EG with the Ca concentration, extracted from the fits.

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  • Figure 10
    Figure 10

    Temperature dependence of the dielectric permittivity for the (a) x=0 and (b) x=0.5 samples for some selected frequencies. Inset: Magnified view of the f=30 kHz curve for the x=0 sample, evidencing the anomaly around TC.

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  • Figure 11
    Figure 11

    (a) Variation in the loss tangent (tanδ) with frequency at different temperatures for the x=0 sample. (b) Relaxation time as a function of the temperature for the x=0 sample. (c) Frequency dependence of tanδ for the x=0.5 sample at different temperatures. (d) Relaxation time as a function of the temperature for the x=0.5 sample. (e), (f) The ɛ vs frequency curves for the x=0 and 0.5 samples, respectively. The red lines in (b) and (d) are the best fits with the Arrhenius equation, while those in (e) and (f) are the best fits with the MW model.

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