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1.
采用磁控溅射方法制备了Pd(3nm)/CoFe(0.8nm)/纳米氧化层/CoFe(fnm)/Cu(4nm)/Pd(5nm)自旋阀底电极薄膜,并用振动样品磁强计对样品的磁性能进行了测量.研究结果表明:纳米氧化层的引入可以使电极薄膜的磁各向异性在退火后从面内转到垂直膜面方向,并且这种强烈的垂直磁各向异性在CoFe有效厚度为2nm时仍能保持.这种具有非多层膜结构、铁磁层较厚、热稳定性较高的底电极有利于基于自旋转移矩的垂直磁各向异性全金属赝自旋阀的发展.  相似文献   

2.
用射频磁控溅射方法制备了一系列颗粒型 N i/Pb不连续多层膜样品 ,并采用 X射线衍射方法表征了样品的微观结构。在铁磁共振实验中 ,观察到了一致进动模 (uniform m ode)和高场光学模 (optical mode)的共振吸收峰。主共振峰和光学模的峰位依赖于外磁场的角度及薄膜厚度。高场光学模的发现表明 ,颗粒型 N i/Pb不连续多层膜存在较强的反铁磁耦合 ,耦合强度随Pb层厚度以指数衰减形式变化。这与面内磁滞回线得到的饱和场随 Pb层厚度的变化关系定性上一致。  相似文献   

3.
采用多靶射频磁控共溅射方法制备了SmCo/Cr薄膜,用XRD和VSM测量了各样品的微结构和矫顽力.结果表明,SmCo膜具有较强的垂直各向异性,当Cr底层溅射时间为5min、SmCo磁性层溅射时间为14min、Co靶溅射功率为220W时,所得到的薄膜垂直矫顽力最大.  相似文献   

4.
对Cr含量为0-23 at%的不同成分系列的CoCr合金薄膜磁畴的研究表明,随着Cr成分增多时其磁各向异性和相关的磁畴结构都敏感地变化。当Cr含量少于17at%时,面内磁化强度为主,并有多种结构形式。超过Cr含量11.2 at%后,少量的垂直磁化强度点畴出现,并随Cr含量增多而增多。Cr含量在17-23 at%的范围内可获得垂直磁各向异性为主的CoCr膜,也可能得到用于高密度垂直磁记录的优良薄膜磁性能。显微照片显示了点畴的尺寸比膜表面的晶粒的或膜断面的晶柱的尺寸都大些。因此,可以得出结论,即其一个自发磁化强度点畴是由一束晶柱或长成的晶粒组成,并都处在单畴状态。  相似文献   

5.
利用磁控溅射在250℃的MgO(220)单晶基片上先后沉积Cr(100 nm)下底层和不同厚度(9~80 nm)的Co-11%W(原子分数)磁性层,二者取向附生生长关系为Cr(112)[111]∥Co-W(1010)[1210]和Cr(112)[110]∥Co-W(1010)[0001].随着膜厚的增加,Co-W在薄膜面内的压应变(ε0)从0.781 3%减小到0.544 5%,相应地其有效磁晶各向异性能一级常数Ke1ff由3.82×106减小到2.58×106erg/cc.该结果表明通过设计磁性层和下底层之...  相似文献   

6.
Ta is often used as a buffer layer in magnetic multilayers. In this study, Ta/Ni81Fe19/Ta multilayers were deposited by magnetron sputtering on sing-crystal Si with a 300-nm-thick SiO2 film. The composition and chemical states at the interface region of SiO2/Ta were studied using the X-ray photoelectron spectroscopy (XPS) and peak decomposition technique. The results show that there is an "intermixing layer" at the SiO2/Ta interface due to a thermodynamically favorable reaction: 15 SiO2 + 37 Ta = 6 Ta2O5 + 5 Ta5Si3. Therefore, the Ta buffer layer thickness used to induce NiFe (111) texture increases.  相似文献   

7.
The hard disk driver (HDD) technology has been loping quickly for recent years. An aerial density of 2 has been demonstrated by Fujitsu and Seagate espectively. To further improve the recording density, the ic effect will be a serious problem tropy of a- alloy thin films in the ordered 0 phase exhibit a perpendicular magnetic anisotropy Ku of the order of 106 J/m3 at room tempera-[1,2] and is very attractive for future high density mag- In the FePt (L10) phase, Fe and Pt atomic c axis, w…  相似文献   

8.
采用改进的溶胶凝胶还原法,利用阳极氧化铝模板(AAO)制备出了不同管壁厚度的Fe纳米管阵列,利用震动样品磁强计测量了平行和垂直于Fe纳米管阵列的磁滞回线,结果表明易磁化轴平行于纳米管的轴向方向,样品具有明显的磁各向异性.  相似文献   

9.
The anisotropy of the microstructure, thermal expansion behavior, corrosion resistance and magnetic properties of AISI 1045 steel was investigated. The distribution of Fe3C lamellae i n the investigation plane parallel to the radial directions of molds was observed to differ from that in the investigation plane perpendicular to the radial directions by transmission electron microscopy. The lattice constants a0 ofα-Fe deduced from the XRD patterns of samples prepared using a sand (S)-mold and cut parallel to the radial direction of t h e m o l d ( S∥) and using a metal (M)-mold and cut parallel to the radial direction (M∥), the corrosion resistance measured using an electrochemical work-station, and the magnetic permeability obtained by vibrating sample magnetometry also indicated the existence of anisotropy in the tested samples. The anisotropic change of corrosion potential (Ecor ), pitting potential (Epit) and magnetic permeability (μ) of the samples was ob-served to depend on the orientation factor F200 ofα-Fe in the measured samples, which is controlled by the distribution of Fe3C lamellae in the eutectoid structure.  相似文献   

10.
[Tb/Fe/Dy]n nano-multilayer films, with precise composition of Tb0.27Dy0.73Fe2, were prepared by the multi-targets magnetron sputtering technique at room temperature (sample A) and 300℃ substrate temperature (sample B). Both of the nano-multilayer films show columnar structures perpendicular to the film plane according to the scanning electron microscopy results. The magnetic hysteresis loops and the giant magnetostriction (GMS) property of the two samples indicate the perpendicular anisotropy in them. In spite of the perpendicular anisotropy, both of the samples present GMS effect. In a very low applied field of 0.18 T, the GMS value in sample B is 89.3 ppm, which is about four times of that in sample A, 23.5 ppm. The good low-field GMS effect in sample B might attribute to the Laves phase of R-Fe2 segregated from the amorphous matrix under the thermal annealing of the substrate. The relation between the magnetization process and GMS property of the perpendicular anisotropy nano-multilayer films is further investigated.  相似文献   

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