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Giant magnetooptic rotations: the role of orbital polarization and explicit correlation effects

机译:巨大的磁光自转:轨道极化的作用和显式相关效应

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An ab initio itinerant-electron calculation for a class of cerium and uranium compounds was performed over the full frequency range studied experimentally. The band structure is obtained from a self-consistent spin-polarized full-potential linearized muffin-tin orbital calculation with a true interstitial. It was found that, for the compounds that display giant Kerr rotations, such a conventional calculation provides magnetooptic behavior very different from that obtained experimentally. This poor agreement was attributed to the presence of a large orbitally driven magnetism totally unlike the magnetism of Ni and Fe, and to the possible importance of explicit correlation effects on approaching heavy fermion behavior. Therefore, explicit orbital polarization was incorporated into the band calculation. This brings about a much better agreement for the ordered magnetic moments but fails to provide adequate agreement for the magnetooptic behavior; furthermore, unlike a calculation including explicit correlation effects, it does not provide agreement with the experimental ordered moment for the incipient heavy fermion CeTe system.
机译:在实验研究的整个频率范围内,对一类铈和铀化合物进行了从头开始的迭代电子计算。能带结构是通过自洽自旋极化全能线性化松饼-锡轨道计算得到的。已经发现,对于显示出巨大克尔旋转的化合物,这种常规计算提供的磁光行为与实验获得的磁光行为非常不同。这种差的协议归因于完全不同于镍和铁的磁性的大轨道驱动磁性的存在,以及显式相关效应对接近重费米子行为的重要性。因此,明确的轨道极化被纳入频带计算。这为有序磁矩带来了更好的一致性,但未能为磁光行为提供足够的一致性。此外,与包括显式相关效应的计算不同,它与初始重费米子CeTe系统的实验有序矩不符。

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