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The magnetic map of FeMn alloy thin films on Co(001) and Co/FeMn/Co(001) trilayers

机译:FeMn合金薄膜在Co(001)和Co / FeMn / Co(001)三层上的磁图

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Recent X-ray magnetic circular dichroism and magneto-optical Kerr effect performed by Matthes et al. [J. Appl. Phys. 93 (2003) 6504] on in situ layered systems of fcc Co and FeMn epitaxially grown onto Cu(001) templates as well as Co/FeMn/Co trilayers display very interesting results. Measurements showed that the magnetic moment on Fe is parallel to the Co magnetization direction whereas, for Mn the XMCD signals are small. In order to explain this behavior ab initio density functional calculations on (Fe_(0.5)Mn_(0.5))_n/Co(001) and Co/(Fe_(0.5)Mn_(0.5))_n/Co(001) have been performed for n varying from 1 to 3. Within generalized gradient corrections the Fe -Mn interfacial alloy, one monolayer thick on Co(001), with ferromagnetic coupling between Fe and Mn corresponds to the ground state whereas the same Fe- Mn monolayer in Co/FeMn/Co presents a magnetic moment of Mn opposite to that of Fe and Co. For all systems investigated we obtain a ferromagnetic polarization between Fe and Co atoms in agreement with the XMCD results. The behavior of the Mn polarization is more complex: an antiferromagnetic polarization between Mn atoms in nearest neighboring FeMn alloy plane is always obtained.
机译:Matthes等人最近完成的X射线磁性圆二色性和磁光Kerr效应。 [J.应用物理93(2003)6504]在外延生长在Cu(001)模板以及Co / FeMn / Co三层上的fcc Co和FeMn的原位分层系统上显示出非常有趣的结果。测量表明,Fe上的磁矩平行于Co磁化方向,而对于Mn,XMCD信号很小。为了解释此行为,已经对(Fe_(0.5)Mn_(0.5))_ n / Co(001)和Co /(Fe_(0.5_Mn_(0.5))_ n / Co(001)进行了从头算密度函数计算n在1到3之间变化。在广义梯度校正中,Fe-Mn界面合金(Co(001)上一个单层厚,Fe和Mn之间具有铁磁耦合)对应于基态,而Co / Mn中相同的Fe-Mn单层FeMn / Co呈现的Mn的磁矩与Fe和Co的磁矩相反。对于所有研究的系统,我们都获得了与XMCD结果一致的Fe和Co原子之间的铁磁极化。 Mn极化的行为更为复杂:始终在最近的FeMn合金平面中获得Mn原子之间的反铁磁极化。

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