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Charge and spin degrees of freedom in A-site ordered YCu3Co4O12 and CaCu3Co4O12

Yi-Ying Chin, Zhiwei Hu, Yuichi Shimakawa, Junye Yang, Youwen Long, A. Tanaka, Liu Hao Tjeng, Hong-Ji Lin, and Chien-Te Chen
Phys. Rev. B 103, 115149 – Published 26 March 2021

Abstract

Using soft x-ray absorption spectroscopy we were able to determine unambiguously the charge and spin states of the transition metal ions in stoichiometric YCu3Co4O12 and CaCu3Co4O12. The trivalent and low-spin nature of both the Cu and Co ions in YCu3Co4O12 makes this correlated system to be effectively a nonmagnetic band semiconductor. The substitution of Y by Ca produces formally tetravalent Co ions but the doped holes are primarily on the oxygen ligands. Concerning the spin degrees of freedom, the trivalent Co ions in YCu3Co4O12 remain low spin upon the Y-Ca substitution, very much unlike the La1xSrxCoO3 system. The tetravalent Co ions in CaCu3Co4O12 are interestingly also in the low-spin state, which then explains the good electrical conductivity of CaCu3Co4O12 since charge exchange between neighboring Co3+ and Co4+ ions will not be hampered by the spin-blockade mechanism that otherwise would be in effect if the Co4+ and Co3+ spin quantum numbers were to differ by more than one-half. We infer that the stability of the Co low-spin state is related to the very short Co-O bond lengths.

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  • Received 28 December 2020
  • Accepted 11 March 2021

DOI:https://doi.org/10.1103/PhysRevB.103.115149

©2021 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Yi-Ying Chin1,*, Zhiwei Hu2, Yuichi Shimakawa3, Junye Yang4, Youwen Long4,5, A. Tanaka6, Liu Hao Tjeng2, Hong-Ji Lin7,†, and Chien-Te Chen7

  • 1Department of Physics, National Chung Cheng University, Chiayi 62102, Taiwan
  • 2Max Planck Institute for Chemical Physics of Solids, Nöthnitzer Strasse 40, 01187 Dresden, Germany
  • 3Institute for Chemical Research, Kyoto University, Kyoto 611-0011, Japan
  • 4Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
  • 5Songshan Lake Materials Laboratory, Dongguan, Guangdong 523808, China
  • 6Quantum Matter Program, Graduate School of Advanced Science and Engineering, Hiroshima University, Higashi-hiroshima 739-8530, Japan
  • 7National Synchrotron Radiation Research Center (NSRRC), 101 Hsin-Ann Road, Hsinchu 30076, Taiwan

  • *Corresponding author: yiyingchin@ccu.edu.tw
  • hjlin@nsrrc.org.tw

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Issue

Vol. 103, Iss. 11 — 15 March 2021

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Images

  • Figure 1
    Figure 1

    Crystal structure of YCu3Co4O12 and CaCu3Co4O12. The Cu ions are coordinated by four oxygens in a square planar symmetry and the Co ions form CoO6 octahedra in a cubic ABO3 perovskite structure.

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  • Figure 2
    Figure 2

    Schematic one-electron energy level diagram for a Co3+ 3d6 [top panel (a)] and a Co4+ 3d5 ion [bottom panel (b)] in octahedral symmetry. The eg and t2g orbital occupations and the total spin quantum number S are indicated for the low-spin (LS), intermediate-spin (IS), and high-spin (HS) configuration.

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  • Figure 3
    Figure 3

    CuL3 XAS spectra of CaCu3Co4O12 (b) and YCu3Co4O12 (c) together with those of CuO as a Cu2+ reference (a) and NaCuO2 as a Cu3+ reference (d). The NaCuO2 spectrum is reproduced from Ref. [28].

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  • Figure 4
    Figure 4

    CoL2,3 XAS spectra of CaCu3Co4O12 (b) and YCu3Co4O12 (c) together with those of CoO (e) as a Co2+ reference, EuCoO3 (d) as a LS Co3+ reference (reproduced from Ref. [9]), and SrCoO3 (a) as a Co4+ reference.

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  • Figure 5
    Figure 5

    Top panel: CoL2,3 XAS spectrum of CaCu3Co4O12 (a, red curve), YCu3Co4O12 scaled by a factor ¾ (a; blue curve), and their difference spectrum (b, black curve). Bottom panel: Enlarge view on the difference spectrum (c,d,e, black curve) together with the theoretical spectrum for a Co4+ LS (c, magenta), IS (d, green), and HS (e, cyan). The inset shows the parameters used in the Co4+ cluster calculations which generated the LS, IS, and HS theoretical spectra. Circles indicate regions of discrepancy between experiment and the calculated spectra.

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  • Figure 6
    Figure 6

    O-K XAS spectra of CaCu3Co4O12 (a), YCu3Co4O12 (b), NaCuO2 (c), EuCoO3 (d), and CuO (e). The NaCuO2 spectrum is reproduced from Ref. [28], and the EuCoO3 spectrum from Ref. [9].

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  • Figure 7
    Figure 7

    Schematic diagram for an inter-site charge exchange between two neighboring Co sites in a mixed valent compound. Top panel: both the Co3+ (S=0) and Co4+ (S=1/2) sites are in the LS (low-spin) state; after the exchange of one electron, both Co ions are still in the LS state. Bottom panel: the Co3+ is LS (S=0) and the Co4 IS (intermediate-spin, S=3/2); after the electron exchange, the Co4+ is LS (S=1/2) and the Co3+ IS (S=1).

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  • Figure 8
    Figure 8

    CuL3 XAS spectra of CaCu3Co4O12 and YCu3Co4O12. Black curves are the raw data taken in the fluorescence yield (FY) mode and red curves are the spectra after correction [27] for the self-absorption effects in the FY.

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