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Spin and charge excitations in the correlated multiband metal Ca3Ru2O7

J. Bertinshaw, M. Krautloher, H. Suzuki, H. Takahashi, A. Ivanov, H. Yavaş, B. J. Kim, H. Gretarsson, and B. Keimer
Phys. Rev. B 103, 085108 – Published 5 February 2021
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Abstract

We use Ru L3-edge resonant inelastic x-ray scattering to study the full range of excitations in Ca3Ru2O7 from meV-scale magnetic dynamics through to the eV-scale interband transitions. This bilayer 4d-electron correlated metal expresses a rich phase diagram, displaying long-range magnetic order below 56 K followed by a concomitant structural, magnetic, and electronic transition at 48 K. In the low-temperature phase, we observe a magnetic excitation with a bandwidth of 30 meV and a gap of 8 meV at the zone center, in excellent agreement with inelastic neutron scattering data. The dispersion can be modeled using a Heisenberg Hamiltonian for a bilayer S=1 system with single-ion anisotropy terms. At a higher energy loss, dd-type excitations show heavy damping in the presence of itinerant electrons, giving rise to a fluorescencelike signal appearing between the t2g and eg bands. At the same time, we observe a resonance originating from localized t2g excitations, in analogy to the structurally related Mott insulator Ca2RuO4. But whereas Ca2RuO4 shows sharp separate spin-orbit excitations and Hund's-rule driven spin-state transitions, here we identify only a single broad asymmetric feature. These results indicate that local intraionic interactions underlie the correlated physics in Ca3Ru2O7, even as the excitations become strongly mixed in the presence of itinerant electrons.

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  • Received 4 December 2020
  • Accepted 25 January 2021

DOI:https://doi.org/10.1103/PhysRevB.103.085108

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI. Open access publication funded by the Max Planck Society.

Published by the American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

J. Bertinshaw1,2,*, M. Krautloher1, H. Suzuki1, H. Takahashi1, A. Ivanov3, H. Yavaş2,†, B. J. Kim1,4,5, H. Gretarsson1,2,‡, and B. Keimer1

  • 1Max Planck Institute for Solid State Research, Heisenbergstrasse 1, D-70569 Stuttgart, Germany
  • 2Deutsches Elektronen-Synchrotron DESY, Notkestraße 85, D-22607 Hamburg, Germany
  • 3Institut Laue-Langevin, 71 Avenue des Martyrs, CS 20156, 38042 Grenoble cedex 9, France
  • 4Department of Physics, Pohang University of Science and Technology, Pohang 790-784, South Korea
  • 5Center for Artificial Low Dimensional Electronic Systems, Institute for Basic Science (IBS), 77 Cheongam-Ro, Pohang 790-784, South Korea

  • *j.bertinshaw@fkf.mpg.de
  • Present address: SLAC National Accelerator Laboratory, 2575 Sand Hill Rd, Menlo Park, CA 94025, USA.
  • hlynur.gretarsson@desy.de

Article Text

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Vol. 103, Iss. 8 — 15 February 2021

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  • Figure 1
    Figure 1

    (a) RIXS energy map taken at T=25 K plots the incident-energy dependence of the energy-loss spectra across the Ru L3 edge. The quasielastic magnon signal and t2g feature at 0.4 eV (horizontal dashed line) resonate around Ei=2838.5 eV, while eg excitations around 3 eV strongly resonate at 2841 eV. At higher energies (6 eV), charge transfer excitations are present. (b) The sample was oriented such that the Ru-O-Ru bonds were aligned 45 to the scattering plane. Outgoing photons kf were detected at a fixed angle of 90 with respect to the incoming beam ki. The momentum transfer was selected by varying the angle θ between ki and the RuO2 planes. (c) Bulk magnetic response of Ca3Ru2O7, with B=0.1 T applied along the b axis. (d) The RIXS energy map conducted above TN [region indicated by a dashed rectangle in (a)] shows a dramatic enhancement of the quasielastic magnetic excitation and an apparent shift of the t2g spectral weight to smaller energy loss. (e)–(g) Comparison of individual RIXS spectra from (a) and (d). The quasielastic contribution has been removed. The dashed vertical line at 0.4 eV lies at the t2g maximum at T=70 K. The arrows identify a second mode with an independent incident-energy response.

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  • Figure 2
    Figure 2

    Ca3Ru2O7 RIXS spectrum, measured at T=25 K and Ei=2838.5 eV at QHKL=(00L) (θ=45), is compared with Ca2RuO4. The Ca2RuO4 data is scaled by a factor of 0.7. Modes associated with spin-wave, t2g, and eg excitations as well as charge transfer are present in both samples. The low-energy splitting of the excitations in Ca2RuO4 are associated with spin-orbit coupling and tetragonal crystal-field terms.

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  • Figure 3
    Figure 3

    (a) The momentum dependence of the RIXS signal below E=200 meV at T=25 K from zone center to zone boundary shows the dispersion of the magnon. (b) The fitted magnon dispersion captured with RIXS corresponds well with inelastic neutron spectroscopy. Solid white lines plot the acoustic and optical modes of the bilayer spin-wave model as discussed in the text, while the color map represents the intensity calculated from the spin-spin correlation function that takes into account instrumental momentum and energy resolutions. The Ca2RuO4 spin-wave position determined from Fig. 2, and model spin wave based on Ref. [25] (dashed white line) are shown for comparison.

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  • Figure 4
    Figure 4

    (a) Temperature dependence of the magnon at the magnetic zone center, corresponding to the spin-wave gap. Above TN, the gap closes and strongly increases in intensity. At T=300 K, weak paramagnetic excitations remain. (b) Fitted magnitude and intensity of the spin-wave gap as a function of temperature. Results reveal that the gap closes at TS, while the bulk of the increase in intensity happens above TN. (c) Momentum dependence of the RIXS spectra at T=25 K collected by varying θ. Each spectrum was normalized to account for self-absorption and shifted vertically for clarity. Overlaid on each spectrum is the data collected at θ=10. (d) Intensity of the t2g features as a function of θ plotted in comparison to the spin-orbit J=2 excitation in Ca2RuO4. Only a moderate increase in spectral weight is observed in Ca3Ru2O7 at low θ.

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