论文标题

共振非弹性X射线散射研究CA $ _3 $ ru $ _2 $ o $ _7 $

Resonant Inelastic X-ray Scattering Study of Ca$_3$Ru$_2$O$_7$

论文作者

von Arx, K., Forte, F., Horio, M., Granata, V., Wang, Q., Das, L., Sassa, Y., Fittipaldi, R., Fatuzzo, C. G., Ivashko, O., Tseng, Y., Paris, E., Vecchione, A., Schmitt, T., Cuoco, M., Chang, J.

论文摘要

我们提出了一项组合的氧$ K $ -EDGE X射线吸收光谱(XAS)和谐振非弹性X射线散射(RIXS)研究双层曲面ca $ _3 $ _3 $ _2 $ o $ o $ $ _7 $。我们对CA $ _3 $ ru $ _2 $ o $ _7 $进行的RIXS实验是在重叠的平面和平面氧气之间进行的,这与顶端具有区别。比较在band-mott绝缘ca $ _2 $ ruo $ _4 $上记录的等效氧$ k $ - 边缘光谱。与Ca $ _2 $ ruo $ _4 $ Spectra相反,其中包含与Mott Physics相关的激发,CA $ _3 $ RU $ _2 $ _2 $ o $ _7 $ SPECTRA功能仅INTRA-intra- $ t_ {2g} $不直接涉及Coulomb Energy量表。如CA $ _2 $ ruo $ _4 $所示,我们解决了两个Intra-$ t_ {2g} $激发ca $ _3 $ ru $ _2 $ o $ $ $ _7 $。此外,CA $ _3 $ ru $ _2 $ o $ _7 $的最低谎言激发显示出了重要的分散体,揭示了一个集体角色与CA $ _2 $ ruo $ _4 $中观察到的集体角色不同。理论建模支持CA $ _3 $ ru $ _2 $ o $ $ _7 $作为具有多粒子角色的磁性横向模式的解释,而Ca $ _2 $ ruo $ _4 $中的相应激发则分配给了延态和横向自旋模式。这些基本差异是根据CA $ _2 $ ruo $ _4 $和Ca $ _3 $ ru $ _2 $ o $ o $ $ _7 $的不等性磁基态表现来讨论这些基本差异。

We present a combined oxygen $K$-edge x-ray absorption spectroscopy (XAS) and resonant inelastic x-ray scattering (RIXS) study of the bilayer ruthenate Ca$_3$Ru$_2$O$_7$. Our RIXS experiments on Ca$_3$Ru$_2$O$_7$ were carried out on the overlapping planar and inter-planar oxygen resonances, which are distinguishable from the apical one. Comparison to equivalent oxygen $K$-edge spectra recorded on band-Mott insulating Ca$_2$RuO$_4$ is made. In contrast to Ca$_2$RuO$_4$ spectra, which contain excitations linked to Mott physics, Ca$_3$Ru$_2$O$_7$ spectra feature only intra-$t_{2g}$ ones that do not directly involve the Coulomb energy scale. As found in Ca$_2$RuO$_4$, we resolve two intra-$t_{2g}$ excitations in Ca$_3$Ru$_2$O$_7$. Moreover, the lowest lying excitation in Ca$_3$Ru$_2$O$_7$ shows a significant dispersion, revealing a collective character differently from what is observed in Ca$_2$RuO$_4$. Theoretical modelling supports the interpretation of this lowest energy excitation in Ca$_3$Ru$_2$O$_7$ as a magnetic transverse mode with multi-particle character, whereas the corresponding excitation in Ca$_2$RuO$_4$ is assigned to combined longitudinal and transverse spin modes. These fundamental differences are discussed in terms of the inequivalent magnetic ground-state manifestations in Ca$_2$RuO$_4$ and Ca$_3$Ru$_2$O$_7$.

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