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Formation of rhombohedral L1_1 CoPt thin film on glass and MgO(111) substrate

机译:在玻璃和MgO(111)衬底上形成菱形L1_1 CoPt薄膜

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摘要

L1_1 type CoPt superstructure, a rhombohedral meta-stable phase, thin films with different thickness (t) were sputtered on glass, Pt/glass, and MgO(111) substrates. Perpendicular magnetic anisotropy (PMA) is obtained as the CoPt films, which are deposited on Pt(111)/glass and MgO substrates. The coercivity (H_c) of CoPt/Pt/glass is higher than that of CoPt/MgO(111) film due to the smaller lattice misfit at CoPt/Pt interface and domain wall impedance at CoPt grain boundary. For the CoPt/Pt/glass and CoPt/MgO films, H_c usually increases with reducing the r from 50 nm to 5 nm. This result could be attributed to the roughness effect at CoPt/Pt and CoPt/MgO interfaces. Without Pt underlayer, CoPt thin film exhibits soft magnetic phase on glass substrate. In this study, higher H_c of about 141 kA/m is shown on 3 nm-thick CoPt film on Pt/glass. The improvement of perpendicular magnetic properties are obtained by replacing the MgO(111) with Pt/glass, inducing high potential of L1_1 CoPt in future applications.
机译:在玻璃,Pt /玻璃和MgO(111)基板上溅射L1_1型CoPt上部结构,菱形亚稳态相,不同厚度(t)的薄膜。垂直磁各向异性(PMA)作为CoPt膜获得,该膜沉积在Pt(111)/玻璃和MgO衬底上。 CoPt / Pt /玻璃的矫顽力(H_c)高于CoPt / MgO(111)薄膜,这是因为CoPt / Pt界面处的晶格失配较小,并且CoPt晶界处的畴壁阻抗较小。对于CoPt / Pt /玻璃和CoPt / MgO薄膜,H_c通常随着r从50 nm减小到5 nm而增加。该结果可以归因于CoPt / Pt和CoPt / MgO界面处的粗糙度效应。没有Pt底层,CoPt薄膜在玻璃基板上显示出软磁相。在这项研究中,在Pt /玻璃上的3 nm厚CoPt膜上显示出大约141 kA / m的较高H_c。通过用Pt /玻璃代替MgO(111),可以提高垂直磁性能,从而在未来的应用中诱导出L1_1 CoPt的高潜力。

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