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The chromium spin density wave: magnetic X-ray scattering studies with polarisation analysis

机译:铬自旋密度波:带有极化分析的X射线磁散射研究

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We report on X-ray magnetic diffraction studies of the spin density wave antiferromagnetism formed in the conduction electron band of chromium. Non-resonant X-ray magnetic scattering was used to directly determine that chromium has zero orbital magnetisation. Furthermore, the azimuthal dependence of this scattering provides unique evidence that chromium forms a linearly polarised wave. In the vicinity of the K absorption edge, resonant X-ray magnetic scattering was observed. A consistent model of the magnetic scattering has been derived from the resonant and non-resonant magnetic amplitudes. The enhancement of the magnetic intensity arises primarily from dipole transitions from the core 1s level to 4p states. Quadrupole transitions to the magnetic 3d states are essentially non-existent due to their sensitivity to (and the absence of) orbital moment. This effect is predicted from atomic considerations of the 3d~5 (L = 0) transition metal ions.
机译:我们报告了在铬的导电电子带中形成的自旋密度波反铁磁性的X射线磁衍射研究。使用非共振X射线磁散射直接确定铬的轨道磁化强度为零。此外,这种散射的方位角依赖性提供了铬形成线性极化波的独特证据。在K吸收边缘附近,观察到共振X射线磁散射。从共振和非共振磁振幅中得出了一致的磁散射模型。磁强度的增强主要来自于从磁芯1s态到4p态的偶极跃迁。由于四极子对轨道力矩的敏感度(和不存在),因此基本上不存在四极跃迁到3d磁性态。从3d〜5(L = 0)过渡金属离子的原子考虑可以预测到这种效果。

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