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Ferromagnetic interaction between Cu ions in the bulk region of Cu-doped ZnO nanowires

机译:Cu掺杂ZnO纳米线块状区域中Cu离子之间的铁磁性相互作用

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摘要

We have studied the electronic structure and the magnetism of Cu-doped ZnOnanowires, which have been reported to show ferromagnetism at room temperature[G. Z. Xing ${et}$ ${al}$., Adv. Mater. {f 20}, 3521 (2008).], by x-rayphotoemission spectroscopy (XPS), x-ray absorption spectroscopy (XAS) and x-raymagnetic circular dichroism (XMCD). From the XPS and XAS results, we find thatthe Cu atoms are in the "Cu$^{3+}$" state with mixture of Cu$^{2+}$ in the bulkregion ($sim$ 100 nm), and that "Cu$^{3+}$" ions are dominant in the surfaceregion ($sim$ 5 nm), i.e., the surface electronic structure of the surfaceregion differs from the bulk one. From the magnetic field and temperaturedependences of the XMCD intensity, we conclude that the ferromagneticinteraction in ZnO:Cu NWs comes from the Cu$^{2+}$ and "Cu$^{3+}$" states inthe bulk region, and that most of the doped Cu ions are magnetically inactiveprobably because they are antiferromagnetically coupled with each other.
机译:我们已经研究了Cu掺杂ZnonanoWare的电子结构和磁性,这些结构据报道在室温下显示铁磁性[g。 z. xing $ {et} $ {al} $。,adv。母娘。 { bf 20},3521(2008)。],通过X射线光学光谱(XPS),X射线吸收光谱(XAS)和X射线磁性圆形二色(XMCD)。从XPS和XAS结果中,我们发现Cu原子在“Cu $ ^ {3 +} $”状态,其中Cu $ ^ {2 +} $中的混合资料($ SIM $ 100nm), “Cu $ ^ {3 +} $”离子在冲浪者中占主导地位($ sim $ 5 nm),即冲浪表面的表面电子结构与散装1不同。从磁场和XMCD强度的温度依存性,我们得出结论,ZnO中的铁磁胺:Cu NWS来自Cu $ ^ {2 +} $和“Cu $ ^ {3 +} $”状态的Inthe Bulk Region,那大多数掺杂的Cu离子是磁性无效的,因为它们是彼此反式磁极耦合的。

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