SPring-8, Japan Atomic Energy Agency, Sayo, Hyogo 679-5148, Japan.
Institute for Materials Research, Tohoku University, Katahira, Sendai 980-8577, Japan.
Nat Commun. 2014 Apr 25;5:3714. doi: 10.1038/ncomms4714.
The evolution of electronic (spin and charge) excitations upon carrier doping is an extremely important issue in superconducting layered cuprates and the knowledge of its asymmetry between electron- and hole-dopings is still fragmentary. Here we combine X-ray and neutron inelastic scattering measurements to track the doping dependence of both spin and charge excitations in electron-doped materials. Copper L3 resonant inelastic X-ray scattering spectra show that magnetic excitations shift to higher energy upon doping. Their dispersion becomes steeper near the magnetic zone centre and they deeply mix with charge excitations, indicating that electrons acquire a highly itinerant character in the doped metallic state. Moreover, above the magnetic excitations, an additional dispersing feature is observed near the Γ-point, and we ascribe it to particle-hole charge excitations. These properties are in stark contrast with the more localized spin excitations (paramagnons) recently observed in hole-doped compounds even at high doping levels.
载流子掺杂时电子(自旋和电荷)激发的演化是超导层状铜酸盐中一个极其重要的问题,其在电子掺杂和空穴掺杂之间的不对称性的相关知识仍然很零散。在这里,我们结合 X 射线和中子非弹性散射测量,来跟踪电子掺杂材料中自旋和电荷激发的掺杂依赖性。铜 L3 共振非弹性 X 射线散射谱表明,磁激发在掺杂时会移向更高的能量。其色散在磁区中心附近变得更陡,并且与电荷激发深度混合,这表明电子在掺杂的金属态中获得了高度迁移的特性。此外,在磁激发之上,在 Γ 点附近观察到一个额外的色散特征,我们将其归因于粒子-空穴电荷激发。这些性质与最近在高掺杂水平下在空穴掺杂化合物中观察到的更局域的自旋激发(paramagnons)形成鲜明对比。