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  • Letter

Emergent interlayer magnetic order via strain-induced orthorhombic distortion in the 5d Mott insulator Sr2IrO4

S. Shrestha, M. Krautloher, M. Zhu, J. Kim, J. Hwang, J. Kim, J.-W. Kim, B. Keimer, and A. Seo
Phys. Rev. B 105, L100404 – Published 9 March 2022
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Abstract

We report a La2CuO4-like interlayer antiferromagnetic order in Sr2IrO4 films with large orthorhombic distortion (>1.5%). The biaxial lattice strain in epitaxial heterostructures of Sr2IrO4/Ca3Ru2O7 lowers the crystal symmetry of Sr2IrO4 from tetragonal (C4) to orthorhombic (C2), guiding the Ir 5d Jeff=1/2 pseudospin moment parallel to the elongated b axis via magnetic anisotropy. From resonant x-ray scattering experiments, we observed an antiferromagnetic order in the orthorhombic Sr2IrO4 film whose interlayer stacking pattern is inverted from that of the tetragonal Sr2IrO4 crystal. This interlayer stacking is similar to that of the orthorhombic La2CuO4, implying that the asymmetric interlayer exchange interactions between a and b directions exceed the anisotropic interlayer pseudodipolar interaction. Our result suggests that strain-induced distortion can provide a delicate knob for tuning the long-range magnetic order in quasi-two-dimensional systems by evoking the competition between the interlayer exchange coupling and the pseudodipolar interaction.

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  • Received 13 September 2021
  • Accepted 22 February 2022

DOI:https://doi.org/10.1103/PhysRevB.105.L100404

©2022 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

S. Shrestha1, M. Krautloher2, M. Zhu3, J. Kim1, J. Hwang3, J. Kim4, J.-W. Kim4, B. Keimer2, and A. Seo1,*

  • 1Department of Physics and Astronomy, University of Kentucky, Lexington, Kentucky 40506, USA
  • 2Max-Planck-Institut für Festkörperforschung, D-70569 Stuttgart, Germany
  • 3Department of Materials Science and Engineering, The Ohio State University, Columbus, Ohio 43210, USA
  • 4Advanced Photon Source, Argonne National Laboratory, Argonne, Illinois 60439, USA

  • *a.seo@uky.edu

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Issue

Vol. 105, Iss. 10 — 1 March 2022

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Images

  • Figure 1
    Figure 1

    (a) A schematic crystal structure of K2NiF4-type oxides. The interlayer exchange interactions Jouta and Joutb share the same interaction paths with the interlayer pseudodipolar interactions Γouta and Γoutb, respectively. (b) Schematic diagrams of two different long-range antiferromagnetic (AFM) stacking patterns in the K2NiF4-type oxides. The AFM-1 type is observed in tetragonal Sr2IrO4 and La2NiO4 crystals, whereas the AFM-2 type is observed in orthorhombic La2CuO4 crystals.

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  • Figure 2
    Figure 2

    (a) A schematic diagram of a Sr2IrO4/Ca3Ru2O7 heterostructure. The red and blue arrows represent compressive and tensile strain directions and magnitudes. (b) X-ray diffraction (0 0 L) scan of a Sr2IrO4/Ca3Ru2O7 heterostructure. The (0 0 12) and (0 0 18) peaks from the Sr2IrO4 thin film are visible. The asterisks [*] indicate the peaks from the Ca3Ru2O7 single-crystal substrate. (c) High-resolution Z-contrast STEM images of a Sr2IrO4/Ca3Ru2O7 heterostructure for two different cross-sectional directions. The red triangles mark the atomically sharp interface between Sr2IrO4 and Ca3Ru2O7. The scale bar is 1 nm.

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  • Figure 3
    Figure 3

    (a) Normalized integrated intensities of the Ir L3-edge (1 0 24) magnetic Bragg peaks of a Sr2IrO4/Ca3Ru2O7 heterostructure as a function of azimuthal angle (Ψ) with σ - π polarization channel. The solid (red) line represents a theoretical calculation for the Jeff=1/2 pseudospin magnetic moment (m) parallel to the crystallographic b axis, as shown in the schematic diagram. Ψ=0 is defined as the crystallographic a axis lying in the scattering plane. The inset shows the same magnetic Bragg peak intensities at selected azimuthal angles. (b) Normalized integrated intensities of the (1 0 24) magnetic Bragg peaks as a function of temperature. The solid (red) line is a power-law fit using the equation I[1TTN]2β, where TN and β are the Néel temperature (∼222 K) and the critical exponent, respectively. (Inset) Normalized integrated intensity vs the reduced temperature (1TTN) in the logarithmic scale. The estimated critical exponent β=0.22 is close to 0.23 corresponding to the 2D XYh4 universality model [33, 34].

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  • Figure 4
    Figure 4

    (a) Ir L3-edge x-ray (1 0 L) and (0 1 L) scans of a Sr2IrO4/Ca3Ru2O7 heterostructure at 6 K. (1 0 16), (1 0 20), (1 0 24), (0 1 18), and (0 1 22) magnetic Bragg peaks are observed. The asterisks [*] indicate the peaks from the Ca3Ru2O7 single-crystal substrate. (b) A schematic phase diagram of AFM stacking orders of Sr2IrO4 as a function of orthorhombic distortion. When α=0, i.e., a tetragonal structure, equivalent twin domains (AFM-1) can coexist. With increasing the orthorhombic distortion (α) up to the critical point (αc), the magnetic domains are just detwinned. With larger orthorhombic distortion than αc, the AFM-2 type stacking order is stabilized, exhibiting the magnetic moment parallel to the b axis and the magnetic Bragg peaks of (104n) and (0 1 4n+2).

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