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Multiferroic behavior in EuTiO3 films constrained by symmetry

P. J. Ryan, G. E. Sterbinsky, Y. Choi, J. C. Woicik, Leyi Zhu, J. S. Jiang, J.-H. Lee, D. G. Schlom, T. Birol, S. D. Brown, P. B. J. Thompson, P. S. Normile, J. Lang, and J.-W. Kim
Phys. Rev. B 101, 180409(R) – Published 29 May 2020

Abstract

We have elucidated the spin, lattice, charge, and orbital coupling mechanism underlying the multiferroic character in tensile-strained EuTiO3 films. Symmetry determined by oxygen octahedral tilting shapes the hybridization between the Eu 4f and the Ti 3d orbitals, and this inhibits predicted Ti displacement proper ferroelectricity. Instead, phonon softening emerges at low temperatures within the pseudocube (110) plane, orthogonal to the anticipated ferroelectric polarization symmetry. Additionally, the magnetic anisotropy is determined by orbital distortion through hybridization between the Ti 3d and the typically isotropic Eu2+4f states. This unique scenario demonstrates the critical role symmetry plays in the coupling of order parameters defining multiferroic behavior.

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  • Received 25 April 2019
  • Revised 10 February 2020
  • Accepted 1 May 2020

DOI:https://doi.org/10.1103/PhysRevB.101.180409

©2020 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

P. J. Ryan1,9,*, G. E. Sterbinsky1, Y. Choi1, J. C. Woicik2, Leyi Zhu3, J. S. Jiang3, J.-H. Lee4, D. G. Schlom4,5, T. Birol6, S. D. Brown7, P. B. J. Thompson7, P. S. Normile8, J. Lang1, and J.-W. Kim1

  • 1Advanced Photon Source, Argonne National Laboratory, Argonne, Illinois 60439, USA
  • 2National Institute of Standards and Technology, Gaithersburg, Maryland 20899, USA
  • 3Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA
  • 4Department of Materials Science and Engineering Cornell University, Ithaca, New York 14853, USA
  • 5Kavli Institute at Cornell for Nanoscale Science, Ithaca, New York 14853, USA
  • 6Department of Chemical Engineering and Materials Science, 421 Washington Avenue, SE, Minneapolis, Minnesota 55455-0132, USA
  • 7Department of Physics, University of Liverpool, Liverpool L69 3BX, United Kingdom
  • 8Departamento de Física Aplicada and Instituto Regional de Investigación Científica Aplicada (IRICA), Universidad de Castilla-La Mancha, 13071 Ciudad Real, Spain
  • 9School of Physical Sciences, Dublin City University, Dublin 9, Ireland

  • *Corresponding author: pryan@anl.gov

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Vol. 101, Iss. 18 — 1 May 2020

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Images

  • Figure 1
    Figure 1

    Reciprocal space scans (along the L direction) of half order reflections resulting from the oxygen octahedral tilt pattern. Absence of the half order (1/21/2¯5/2) indicates that the film has a single-type tilt domain. Cartoons illustrating (left) the ETO pseudocubic unit cell showing G-AFM order with all three coexisting spin-ordering interactions and (right) the biaxial strain and single oxygen-related tilt pattern imposed by the DSO (110) substrate.

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  • Figure 2
    Figure 2

    (a) Ti K-edge near-edge spectra with linear polarization at 5 and 275 K. (b) Expanded plots of the spectral intensities of the eg preedge peak contrasting the temperature dependence of polarization parallel to both in-plane [100] and out-of-plane [001] as depicted in the inset. (c) Cartoon illustration of the relative incident polarization (yellow arrows) with low-temperature phonon softening effect along [001] (cyan arrow). (d) Azimuthal-temperature dependence of eg preedge intensity along both e||[110] and e||[1¯10]. (e) Cartoon displaying the relative incident geometries with the arrow indicating increased softening. (f) Temperature dependence of the eg preedge intensity with the polarization along the [110] and [1¯10]. (g) Temperature dependence of the in-plane film resistance. The inset shows the comparison between other strain states. (h) Cartoon showing the aggregate relative orientation of Ti phonon softening along the cube diagonal with respect to the oxygen tilting within the (110) plane.

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  • Figure 3
    Figure 3

    (a) Temperature-dependent XRMS-scattering intensity of the (003)ETO reflection at the Eu LII edge indicative of FM spin order. The inset of the bottom left corner illustrates the horizontal-scattering experimental configuration (π-σ), and the top right shows resonant enhancement (background subtracted) above and below Tc. (b) Energy scans at the (003)ETO reflection in (π-π) geometry where the charge-scattering intensity can interfere with the magnetic scattering. The in- and out-of-phase interferences of magnetic and charge scatterings are dependent on the aligned spin direction. (c) Field-dependent sweeps with fixed energy in (π-π) showing clear FM hysteresis loops. Data are offset for clarity. With the applied field along the easy magnetic axis [1¯10], the hysteresis loop shows a minimum coercivity. Along the [010] and close to the [110], the intensity difference between positive and negative field directions decreases, and the loop broadens. The inset images illustrate, regardless of changes in the field direction by sample rotation, the spins stay within the easy axis [1¯10]. (d) A cartoon model illustrating the relative orientation of the oxygen Oh tilting, Ti phonon softening, and uniaxial magnetic anisotropy.

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