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Direct Imaging of Orbitals in Quantum Materials

Invited

Abstract

The search for new quantum materials with novel properties is often focused on materials containing transition-metal or rare-earth elements. The presence of the atomic-like d or f orbitals provides a fruitful playground to generate novel phenomena and understanding the behavior of those d and f electrons is essential for designing and tuning new materials. Therefore, identifying the d or f orbitals that actively participate in the formation of the ground state is crucial. So far, these orbitals have mostly been deduced from optical, X-ray and neutron spectroscopies in which spectra must be analyzed using theory or modelling. This, however, is also a challenge in itself, since ab-initio calculations hit their limits due to the many-body nature of the problem.

Here we developed a new experimental method that circumvents the need for involved analysis and instead provides the information as measured. With this technique, we can make a direct image of the active orbital and determine what the atomic-like object looks like in a real solid. The method, s-core-level non-resonant inelastic X-ray scattering (s-NIXS), relies on high momentum transfer in the inelastic scattering process, which is necessary for dipole-forbidden terms to gain spectral weight. To demonstrate the strength of the technique, we imaged the text-book example, x2-y2/3x2-r2 hole orbital of the Ni2+ ion in NiO single crystal [1]. We will present the basic principles of s-NIXS and its experimental implementation. We will also show how we can apply this technique to unveil the active orbitals in complex oxides as well as to determine the orbital character in highly metallic systems such as elemental Cr, Fe, and Ni.

[1] H. Yavas, M. Sundermann, K. Chen, A. Amorese, A. Severing, H. Gretarsson, M.W. Haverkort, L.H. Tjeng,
Nature Physics (2019) ; https://doi.org/10.1038/s41567-019-0471-2.

Presenters

  • Liu Tjeng

    Max Planck Inst, Max-Planck Institute for Chemical Physics of Solids Dresden, Max Planck Institute for Chemical Physics of Solids, Dresden, Germany, Max Planck Institute for Chemical Physics of Solids

Authors

  • Liu Tjeng

    Max Planck Inst, Max-Planck Institute for Chemical Physics of Solids Dresden, Max Planck Institute for Chemical Physics of Solids, Dresden, Germany, Max Planck Institute for Chemical Physics of Solids

  • Hasan Yavas

    DESY, Hamburg, Germany

  • Martin Sundermann

    Institute of Physics II, University of Cologne, Physics 2, University of Cologne, Germany, Max Planck Institute for Chemical Physics of Solids

  • Brett Leedahl

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

  • Kai Chen

    Physics 2, University of 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, Physics 2, University of Cologne, Germany, University of Cologne

  • Hlynur Gretarsson

    DESY, Hamburg, Germany, Deutsches Elektronen-Synchrotron (DESY)

  • Maurits Haverkort

    Institute for Theoretical Physics, Heidelberg University, Institute for theoretical physics, Institute of Theoretical Physics, University of Heidelberg, Theoretical Physics, Heidelberg University, Germany, Heidelberg University