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首页> 外文期刊>Physical review. B, Condensed Matter And Materals Physics >Resonant inelastic x-ray scattering studies of magnons and bimagnons in the lightly doped cuprate La_(2-x)Sr_xCuO_4
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Resonant inelastic x-ray scattering studies of magnons and bimagnons in the lightly doped cuprate La_(2-x)Sr_xCuO_4

机译:轻掺杂铜酸盐La_(2-x)Sr_xCuO_4中的强子和双强子的共振非弹性x射线散射研究

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摘要

We investigated the doping dependence of magnetic excitations in the lightly doped cuprate La_(2-x)Sr_xCuO_4 via combined studies of resonant inelastic x-ray scattering (RIXS) at the Cu L_3, edge and theoretical calculations. With increasing doping, the magnon dispersion is found to be essentially unchanged, but the spectral width broadens and the spectral weight varies differently at different momenta. Near the Brillouin zone center, we directly observe bimagnon excitations that possess the same energy scale and doping dependence as previously observed by Raman spectroscopy. They disperse weakly in energy-momentum space, and they are consistent with a bimagnon dispersion that is renormalized by the magnon-magnon interaction at the zone center.
机译:我们通过对Cu L_3处的共振非弹性X射线散射(RIXS),边缘和理论计算的综合研究,研究了轻掺杂的铜酸盐La_(2-x)Sr_xCuO_4中磁激发的掺杂依赖性。随着掺杂的增加,发现磁振子的色散基本不变,但是光谱宽度变宽并且光谱权重在不同的时刻不同地变化。在布里渊区中心附近,我们直接观察到双磁子激发,该双磁子激发具有与以前通过拉曼光谱法观察到的相同的能级和掺杂依赖性。它们在能量动量空间中的扩散较弱,并且与通过区域中心的磁振子-磁振子相互作用重新归一化的双磁振子弥散相一致。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics 》 |2018年第15期| 155144.1-155144.8| 共8页
  • 作者单位

    Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory and Stanford University,2575 Sand Hill Road, Menlo Park California 94025, USA;

    Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory and Stanford University,2575 Sand Hill Road, Menlo Park California 94025, USA;

    SwissFEL and Laboratory for Micro and Nanotechnology, Paul Scherrer Institut, 5232 Villigen PSI, Switzerland;

    Swiss Light Source, Paul Scherrer lnstitut, 5232 Villigen PSI, Switzerland;

    Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory and Stanford University,2575 Sand Hill Road, Menlo Park California 94025, USA;

    Swiss Light Source, Paul Scherrer lnstitut, 5232 Villigen PSI, Switzerland;

    Swiss Light Source, Paul Scherrer lnstitut, 5232 Villigen PSI, Switzerland;

    Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory and Stanford University,2575 Sand Hill Road, Menlo Park California 94025, USA;

    Laboratoire PROMES-CNRS (UPR-8521), Universite de Perpignan Via Domitia, Rambla de la Thermodynamique,Tecnosud, 66100 Perpignan, France;

    Department of Physics, Technion-Israel Institute of Technology, Haifa 32000, Israel;

    Swiss Light Source, Paul Scherrer lnstitut, 5232 Villigen PSI, Switzerland;

    Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory and Stanford University,2575 Sand Hill Road, Menlo Park California 94025, USA;

    Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory and Stanford University,2575 Sand Hill Road, Menlo Park California 94025, USA ,Geballe Laboratory for Advanced Materials, Stanford University, Stanford, California 94305, USA;

    Swiss Light Source, Paul Scherrer lnstitut, 5232 Villigen PSI, Switzerland;

    Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory and Stanford University,2575 Sand Hill Road, Menlo Park California 94025, USA ,Geballe Laboratory for Advanced Materials, Stanford University, Stanford, California 94305, USA;

    Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory and Stanford University,2575 Sand Hill Road, Menlo Park California 94025, USA;

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