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Structure and giant magnetoresistance behaviour of Co-Cu/Cu multilayers electrodeposited under various deposition conditions

机译:不同沉积条件下电沉积Co-Cu / Cu多层膜的结构和巨磁致电阻行为

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Electrodeposited Co-Cu/Cu multilayers were prepared under a variety of deposition conditions on either a polycrystalline Ti foil or on a silicon wafer covered by a Ta buffer and a Cu seed layer. X-ray diffraction (XRD) revealed a strong (111) texture for all multilayers with clear satellite peaks for the multilayers on Si/Ta/Cu substrates, in some cases for up to three reflections. Cross-sectional (1) transmission electron microscopy investigations indicated a much more uniform multilayer structure on the Si/Ta/Cu substrates. The bilayer periods from XRD satellite reflections were in reasonable agreement with nominal values. An analysis of the overall chemical composition of the multilayers gave estimates of the sublayer thickness changes due to the Co-dissolution process during the Cu deposition pulse. The XRD lattice spacing data indicated a behaviour close to a simple "multilayer" Vegard's law which was, however, further refined by taking into account elastic strains as well. In agreement with the structural studies, magnetoresistance data also indicated the formation of more perfect multilayers on the smooth Si/Ta/Cu substrates. An analysis of the magnetoresistance behaviour revealed the presence of superparamagnetic (SPM) regions in the magnetic layers. The contribution of these SPM regions to the total observed giant magnetoresistance was found to be dominating under certain deposition conditions, e.g., for magnetic layer thicknesses less than 1 nm (about 5 monolayers).
机译:在多种沉积条件下,在多晶Ti箔上或在Ta缓冲层和Cu籽晶层覆盖的硅片上,制备电沉积的Co-Cu / Cu多层膜。 X射线衍射(XRD)显示,所有多层均具有很强的(111)织构,并且在Si / Ta / Cu衬底上的多层中具有清晰的卫星峰,在某些情况下最多可反射3次。截面(1)的透射电子显微镜研究表明,Si / Ta / Cu基板上的多层结构更为均匀。 XRD卫星反射的双层周期与标称值在合理范围内一致。对多层的整体化学成分的分析给出了由于在铜沉积脉冲期间的共溶解过程而引起的亚层厚度变化的估计。 XRD晶格间距数据表明其行为接近简单的“多层”维加德定律,但是通过考虑弹性应变进一步完善了该定律。与结构研究一致,磁阻数据还表明在光滑的Si / Ta / Cu衬底上形成了更完美的多层。对磁阻行为的分析表明,磁性层中存在超顺磁性(SPM)区域。发现在某些沉积条件下,例如对于小于1nm的磁性层厚度(约5个单层),这些SPM区域对总的观察到的巨磁致电阻的贡献占主导。

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