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The Origin of Ising Magnetism in Ca<sub>3</sub>O<sub>2</sub>O<sub>6</sub> Unveiled by Orbital Imaging

ORAL

Abstract

One-dimensional CoO6 chains in Ca3Co2O6 give rise to an Ising-like magnetism with an intriguing quantum tunneling staircase structure in its magnetization. To resolve the underlying local electronic configuration of the Co ions in this material we applied s-core-level non-resonant inelastic x-ray scattering (s-NIXS), a new technique that is capable of imaging the shape of the 3d orbitals in real space. The orbital shapes that we found established that both Co sites (octahedral and trigonal prismatic) are in the 3+ valence state (i.e. 3d6); the trigonal Co site has a high-spin configuration, while the octahedral Co site is low spin. We directly "see" that it is the complex d2 orbital that is stabilized by the prismatic trigonal coordination, which naturally explains the Ising magnetism in the system. Utilizing this ability to image electron orbitals, and thus directly relating the orbital occupation with the local crystal structure—without the need for theoretical modeling—is essential for modeling magnetic properties. This is especially true in situations where one would like to make use of the delicate balance of competing interactions to stabilize a particular orbital state for a desired or optimized physical property. This work is published in Nature Communications.

Presenters

  • Brett Leedahl

    Max Planck Institute for Chemical Physics of Solids

Authors

  • Brett Leedahl

    Max Planck Institute for Chemical Physics of Solids

  • Martin Sundermann

    Max Planck Institute for Chemical Physics of Solids, Institute of Physics II, University of Cologne, Cologne, Germany

  • Andrea Amorese

    Max Planck Institute for Chemical Physics of Solids, Max Planck Institute for Chemical Physics of Solids (Dresden, Germany)

  • Andrea Severing

    Institute of Physics II, University of Cologne, Intitute of Physics II, University of Cologne, University of Cologne, Institute of Physics II, University of Cologne (Germany), Institute of Physics II, University of Cologne, Cologne, Germany

  • Hlynur Gretarsson

    PETRA III, Deutsches Elektronen-Synchrotron (DESY), Petra III, DESY

  • Lunyong Zhang

    Max Planck Institute for Chemical Physics of Solids

  • Alexander Komarek

    Max Planck Institute for Chemical Physics of Solids, Max Planck Institute for Chemical Physics of Solids (MPI CPfS), Max Planck Institute

  • Antoine Maignan

    Laboratoire CRISMAT

  • Maurits Wim Haverkort

    Institute for Theoretical Physics, Heidelberg University, Heidelberg University, Institute for theoretical Physics, Heidelberg University (Germany), Institute for theoretical Physics, University of Heidelberg

  • Liu Tjeng

    Max Planck Institute for Chemical Physics of Solids, Max Planck Institute for Chemical Physics of Solids, Dresden, Germany, Max Planck Institute for Chemical Physics of Solids (Dresden, Germany), Max Planck Institute for Chemical Physics of Solids (MPI CPfS), Max-Planck Institute for Chemical Physics of Solids