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Dispersive magnetic and electronic excitations in iridate perovskites probed by oxygen K-edge resonant inelastic x-ray scattering

机译:氧钾边缘共振非弹性X射线散射探测铱酸盐钙钛矿中的分散性磁和电子激发

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摘要

Resonant inelastic x-ray scattering (RIXS) experiments performed at the oxygen K edge on the iridate perovskites Sr_2IrO_4 and Sr_3Ir_2O_7 reveal a sequence of well-defined dispersive modes over the energy range up to ~0.8 eV. The momentum dependence of these modes and their variation with the experimental geometry allows us to assign each of them to specific collective magnetic and/or electronic excitation processes, including single and bimagnons, and spin-orbit and electron-hole excitons. We thus demonstrate that dispersive magnetic and electronic excitations are observable at the O K edge in the presence of the strong spin-orbit coupling in the 5d shell of iridium and strong hybridization between Ir 5d and O 2p orbitals, which confirm and expand theoretical expectations. More generally, our results establish the utility of O K-edge RIXS for studying the collective excitations in a range of 5d materials that are attracting increasing attention due to their novel magnetic and electronic properties. Especially, the strong RIXS response at O K edge opens up the opportunity for investigating collective excitations in thin films and heterostructures fabricated from these materials.
机译:在铱酸盐钙钛矿Sr_2IrO_4和Sr_3Ir_2O_7的氧K边缘进行的共振非弹性X射线散射(RIXS)实验揭示了在能量范围高达〜0.8 eV时,一系列明确定义的色散模式。这些模式的动量依赖性及其随实验几何形状的变化使我们能够将它们分配给特定的集体磁和/或电子激发过程,包括单和双磁子,自旋轨道和电子空穴激子。因此,我们证明,在铱的5d壳中存在强自旋轨道耦合以及Ir 5d和O 2p轨道之间的强杂化的情况下,在O K边缘处可观察到分散的磁和电子激发,这证实并扩展了理论上的期望。更一般而言,我们的结果建立了O K-edge RIXS在研究5d材料中的集体激发方面的效用,这些材料由于其新颖的磁性和电子性质而受到越来越多的关注。特别是,在O K边缘的强烈RIXS响应为研究由这些材料制成的薄膜和异质结构中的集体激发提供了机会。

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  • 来源
    《Physical review 》 |2018年第4期| 041102.1-041102.6| 共6页
  • 作者单位

    Research Department Synchrotron Radiation and Nanotechnology, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland;

    Research Department Synchrotron Radiation and Nanotechnology, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland;

    Research Department Synchrotron Radiation and Nanotechnology, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland;

    Research Department Synchrotron Radiation and Nanotechnology, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland;

    Research Department Synchrotron Radiation and Nanotechnology, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland;

    Institute of Physics, Ecole Polytechnique Federate de Lausanne (EPFL), CH-1015 Lausanne, Switzerland;

    Research Department Synchrotron Radiation and Nanotechnology, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland;

    London Centre for Nanotechnology and Department of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT, United Kingdom;

    School of Physics and Astronomy, The University of Edinburgh, James Clerk Maxwell Building, Mayfield Road,Edinburgh EH9 2TT, United Kingdom;

    Laboratory for Quantum Magnetism, Institute of Physics, Ecole Polytechnique Federale de Lausanne (EPFL),CH-1015 Lausanne, Switzerland;

    Research Department Synchrotron Radiation and Nanotechnology, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland;

    ISIS Neutron Spallation Source, Rutherford Appleton Laboratory (RAL), Harwell Campus, Didcot OX11 0QX, United Kingdom,London Centre for Nanotechnology and UCL Centre for Materials Discovery, University College London, 17-19 Gordon Street,London WC1H 0AH, United Kingdom;

    Institute of Physics, Ecole Polytechnique Federate de Lausanne (EPFL), CH-1015 Lausanne, Switzerland;

    London Centre for Nanotechnology and Department of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT, United Kingdom;

    Laboratory for Quantum Magnetism, Institute of Physics, Ecole Polytechnique Federale de Lausanne (EPFL),CH-1015 Lausanne, Switzerland;

    Research Department Synchrotron Radiation and Nanotechnology, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland;

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