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Localized and mixed valence state of Ce 4f in superconducting and ferromagnetic CeO1xFxBiS2 revealed by x-ray absorption and photoemission spectroscopy

T. Sugimoto, D. Ootsuki, E. Paris, A. Iadecola, M. Salome, E. F. Schwier, H. Iwasawa, K. Shimada, T. Asano, R. Higashinaka, T. D. Matsuda, Y. Aoki, N. L. Saini, and T. Mizokawa
Phys. Rev. B 94, 081106(R) – Published 17 August 2016

Abstract

We have performed Ce L3-edge x-ray absorption spectroscopy (XAS) and Ce 4d4f resonant photoemission spectroscopy (PES) on single crystals of CeO1xFxBiS2 for x=0.0 and 0.5 in order to investigate the Ce 4f electronic states. In Ce L3-edge XAS, a mixed valence of Ce was found in the x=0.0 sample, and F doping suppressed it, which is consistent with the results on polycrystalline samples. As for resonant PES, we found that the Ce 4f electrons in both x=0.0 and 0.5 systems respectively formed a flat band at 1.0 and 1.4 eV below the Fermi level and there was no contribution to the Fermi surfaces. Interestingly, Ce valence in CeOBiS2 deviates from Ce3+ even though Ce 4f electrons are localized, indicating the Ce valence is not in a typical valence fluctuation regime. We assume that localized Ce 4f in CeOBiS2 is mixed with unoccupied Bi 6pz, which is consistent with a previous local structural study. Based on the analysis of the Ce L3-edge XAS spectra using Anderson's impurity model calculation, we found that the transfer integral becomes smaller, increasing the number of Ce 4f electrons upon the F substitution for O.

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  • Received 29 March 2016
  • Revised 28 July 2016

DOI:https://doi.org/10.1103/PhysRevB.94.081106

©2016 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

T. Sugimoto1,2, D. Ootsuki1,2, E. Paris3,4, A. Iadecola5, M. Salome5, E. F. Schwier6, H. Iwasawa6, K. Shimada6, T. Asano7, R. Higashinaka7, T. D. Matsuda7, Y. Aoki7, N. L. Saini3, and T. Mizokawa8

  • 1Department of Physics & Complexity Science and Engineering, University of Tokyo, 5-1-5 Kashiwanoha 277-8561, Japan
  • 2Institute for Solid State Physics, University of Tokyo, 5-1-5 Kashiwanoha 277-8561, Japan
  • 3Dipartimento di Fisica, Universitá di Roma “La Sapienza”, Piazzale Aldo Moro 2, 00185 Roma, Italy
  • 4Center for Life NanoScience@Sapienza, Istituto Italiano di Tecnologia, V. le Regina Elena 291, 00185 Rome, Italy
  • 5ESRF–The European Synchrotron, 71 avenue des Martyrs, 38043 Grenoble Cedex 9, France
  • 6Hiroshima Synchrotron Radiation Center, Hiroshima University, Hiroshima 739-0046, Japan
  • 7Department of Physics, Tokyo Metropolitan University, Tokyo 192-0397, Japan
  • 8Department of Applied Physics, Waseda University, Tokyo 169-8555, Japan

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Issue

Vol. 94, Iss. 8 — 15 August 2016

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Images

  • Figure 1
    Figure 1

    (a) Real space image of micro x-ray absorption near edge structure (μXANES) at the Ce L3 edge (5.732 keV) on CeOBiS2 and (b) on CeO0.5F0.5BiS2. (c) Normalized XAS spectra of CeOBiS2 and CeO0.5F0.5BiS2. The background (arctangent function) is denoted by the dotted-dashed line. The spectra after background subtraction are also shown in the inset.

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  • Figure 2
    Figure 2

    (a) CIS plot of CeO0.5F0.5BiS2. Fermi surfaces of CeO0.5F0.5BiS2 taken (b) at 120.3 eV on resonance, (c) at 115.4 eV off resonance, and (d) at 30 eV. The ARPES intensities are integrated within ±50 meV with respect to EF. (e) Cut along MΓX with off-resonant hν and (e) its second derivative, (f) cut with on-resonant photon energy, (i) EDCs integrated along MΓX for both off- and on-resonant hν, and the inset shows the expanded view near EF on CeOBiS2. (g), (g), (h), and (j) are the same as (e), (e), (d), and (i) but on CeO0.5F0.5BiS2.

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  • Figure 3
    Figure 3

    (a) Schematic diagram of the effective transfer integral T. Ce L3-edge XAS experimental results on single crystal CeO1xFxBiS2 and corresponding impurity model calculations at (a) x=0.0 and (b) x=0.5. The energy positions of 4f1 and 4f0 are shown by vertical lines. The effective transfer integral (T) and number of Ce 4f electrons (nf) estimated by Anderson's impurity model calculation are also shown here.

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