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Spin-state ordering and intermediate states in the mixed-valence cobalt oxyborate Co3O2BO3 with spin crossover

E. Granado, C. W. Galdino, B. D. Moreno, G. King, and D. C. Freitas
Phys. Rev. B 109, 094115 – Published 22 March 2024

Abstract

Spin-state ordering—a periodic pattern of ions with different spin-state configurations along a crystal lattice—is a rare phenomenon, and its possible interrelation with other electronic degrees of freedom remains little explored. Here we perform a structural investigation of the mixed-valence Co homometallic ludwigite Co22+Co3+O2BO3. A superstructure consistent with a long-range Co3+ spin-state ordering is observed between T4=580 K and T3=510 K. Intermediate states with mesoscopic correlations are detected below T3 down to T1=480 K with a change of dimensionality at T2=495 K. The spin-state correlations are connected to the charge sector as revealed by the abrupt changes in the electrical resistance at T1 and T2. The evolution of the structural parameters below T1 indicate that the spin crossover is ignited by a moderate degree of thermally induced Co2+ and Co3+ charge disorder. Charge and spin-state degrees of freedom can be interrelated in mixed-valence spin-crossover materials, leading to sharp transitions involving intermediate spin-state and charge-correlated states at the mesoscale.

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  • Received 4 September 2023
  • Revised 16 February 2024
  • Accepted 11 March 2024

DOI:https://doi.org/10.1103/PhysRevB.109.094115

©2024 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

E. Granado1,*, C. W. Galdino1,†, B. D. Moreno2, G. King2, and D. C. Freitas3

  • 1Gleb Wataghin Institute of Physics, University of Campinas (UNICAMP), Campinas, São Paulo 13083-859, Brazil
  • 2Canadian Light Source Inc., 44 Innovation Boulevard, Saskatoon, Saskatchewan S7N 2V3, Canada
  • 3Instituto de Física, Universidade Federal Fluminense, Campus da Praia Vermelha, Niterói, RJ 24210-346, Brazil

  • *granado@unicamp.br
  • Present address: Swiss Light Source, Paul Scherrer Institute, 5232 Villigen-PSI, Switzerland.

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Issue

Vol. 109, Iss. 9 — 1 March 2024

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Images

  • Figure 1
    Figure 1

    Representative x-ray powder diffraction profile and Rietveld fit at T=300 K (λ=0.2265 Å, Rw=4.17%). Cross symbols represent the experimental data and the green solid line is the simulated profile after the refinement. The raw difference data is the solid cyan line. The expected Bragg positions for the main Co3O2BO3 ludwigite and the minor Co3O4 impurity phases (1.7% weight fraction) are given in red and blue short vertical bars, respectively.

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  • Figure 2
    Figure 2

    (a) Average Co(n)-O distances for n=14 obtained from the refined atomic positions and lattice parameters. (b) Average CoO distances within the 313 and 424 three-legged ladders.

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  • Figure 3
    Figure 3

    (a)–(h) Azimuthal (ϕ) scans of the superstructure 441 reflection (c-doubled unit cell) around the [110] axis at selected temperatures.

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  • Figure 4
    Figure 4

    Temperature dependence of the integrated intensity of the (ϕ) scans in linear (a) and logarithmic (b) scales. The linewidths are given in (c). The identified transition temperatures, T1=480 K, T2=495 K, T3=510 K, and T4=580 K, are marked as vertical dashed lines.

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  • Figure 5
    Figure 5

    (a) ab-plane projection of the crystal structure of Co3O2BO3 at T=525 K (Pbnm space group). (b) Detailed view of the Co(4a)-Co(2)-Co(4b) (424) three-legged ladders. The main difference of the superstructure with respect to the regular ludwigite structure (Pbam space group) is the splitting of the Co(4) site of the latter into inequivalent Co(4a) and Co(4b) sites that are alternately stacked along c, leading to a doubled unit cell [thin black lines in (a) and (b)]. The various oxygen (red) and boron (green) sites are drawn with the same colors for simplicity. This figure was produced using VESTA [63].

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  • Figure 6
    Figure 6

    Reciprocal-space scans around the 441 superlattice peak along the h (a), k (b) and ldirections (c) at selected temperatures. (d) Temperature dependence of the 441 peak area in log scale, obtained from the h, k, and l scans. A detailed view of (d) in linear scale below 505 K is given in (e). Solid straight lines are guides to the eyes. (f) Temperature dependence of the 441 peak linewidths of the reciprocal-space scans. The anisotropic correlation lengths ξa, ξb, and ξc, extracted from data of (f) after decovolution of the instrumental widths, are given in (g). The transition temperatures T1T3 are marked in (d-g) as vertical dashed lines.

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  • Figure 7
    Figure 7

    (a)–(c) Reciprocal-space k scans around the 441 reflection at T=513 K (a), T=506 K (b) and T=499 K (c) (symbols), and fits to a pseudo-Voigt lineshape, PV(kk0)=xL(kk0)+(1x)G(kk0) (solid lines), where L and G are Lorentzian and Gaussian functions, respectively, and the Lorentzian weight factor x is restrained to range between 0 and 1. (d) Temperature dependence of x obtained from the fits illustrated in (a-c). (e-h) Reciprocal-space l scans around the 441 reflection at T=513 K (e), T=506 K (f), T=499 K (g), and T=492 K (h) (symbols), and fits to a pseudo-Voigt lineshape (solid lines). (i) Temperature dependence of x obtained from the fits illustrated in (e-h).

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  • Figure 8
    Figure 8

    Electrical resistance of a needle-shaped crystal of Co3O2BO3 along the c direction (solid line). The dashed line is the extrapolated behavior between T1 and T2.

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