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首页> 外文期刊>Journal of Physics. Condensed Matter >Magnetization reversal in a preferred oriented (111) L1_0 FePt grown on a soft magnetic metallic glass for tilted magnetic recording
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Magnetization reversal in a preferred oriented (111) L1_0 FePt grown on a soft magnetic metallic glass for tilted magnetic recording

机译:在倾斜磁记录的软磁金属玻璃上生长的取向较好的(111)L1_0 FePt的磁化反转

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摘要

L1_0 FePt is an important material for the fabrication of high density perpendicular recording media, but the ultrahigh coercivity of L1_0 FePt restricts its use. Tilting of the magnetic easy axis and the introduction of a soft magnetic underlayer can solve this problem. However, high temperature processing and the requirement of epitaxial growth conditions for obtaining an L1_0 FePt phase are the main hurdles to be overcome. Here, we introduce a bilayered magnetic structure ((111) L1_0 FePt/glassy Fe _(71)Nb _4Hf _3Y _2B _(20)/SiO_2/Si) in which the magnetic easy axis of L1_0 FePt is tilted by 36°from the film plane and epitaxial growth conditions are not required. The soft magnetic underlayer not only promotes the growth of L1_0 FePt with the preferred orientation but also provides an easy cost-effective microanopatterning of recording bits. A detailed magnetic characterization of the bilayered structure in which the thickness of (111) L1_0 FePt with the soft magnetic Fe_(71)Nb_4Hf_3Y_2B_(20) glassy underlayer varied from 5 to 60nm is carried out in an effort to understand the magnetization switching mechanism. The magnetization switching behavior is almost the same for bilayered structures in which FePt layer thickness is >10nm (greater than the domain wall thickness of FePt). For FePt film 10nm thick, magnetization reversal takes place in a very narrow field range. Magnetization reversal first takes place in the soft magnetic underlayer. On further increase in the reverse magnetic field, the domain wall in the soft magnetic layer compresses at the interface of the hard and soft layers. Once the domain wall energy becomes sufficiently large to overcome the nucleation energy of the domain wall in L1_0 FePt, the magnetization of the whole bilayer is reversed. This process takes place quickly because the domain walls in the hard layer do not need to move, and the formation of a narrower domain wall may not be favorable energetically. Our results showed that the present bilayered structure is very promising for the fabrication of tilted bit-patterned magnetic recording media.
机译:L1_0 FePt是制造高密度垂直记录介质的重要材料,但是L1_0 FePt的超高​​矫顽力限制了其使用。磁易轴的倾斜和软磁衬层的引入可以解决此问题。然而,高温处理和获得L1_0 FePt相的外延生长条件的要求是要克服的主要障碍。在这里,我们介绍了一种双层磁性结构((111)L1_0 FePt /玻璃状Fe _(71)Nb _4Hf _3Y _2B _(20)/ SiO_2 / Si),其中L1_0 FePt的易磁化轴从轴上倾斜36°。不需要膜平面和外延生长条件。软磁衬层不仅可以促进L1_0 FePt以最佳取向生长,而且还提供了一种经济高效的微型/纳米记录位记录方法。为了理解磁化切换机理,对其中具有软磁性Fe_(71)Nb_4Hf_3Y_2B_(20)玻璃状下层的(111)L1_0 FePt的厚度从5nm改变到60nm的双层结构进行了详细的磁性表征。对于FePt层厚度> 10nm(大于FePt的畴壁厚度)的双层结构,磁化切换行为几乎相同。对于10nm厚的FePt膜,磁化反转发生在非常窄的场范围内。磁化反转首先发生在软磁性底层中。随着反向磁场的进一步增加,软磁性层中的畴壁在硬层和软层的界面处压缩。一旦畴壁能量变得足够大以克服L1_0 FePt中畴壁的形核能,整个双层的磁化强度就会反转。由于不需要移动硬层中的畴壁,因此该过程很快发生,并且较窄的畴壁的形成可能在能量上不是有利的。我们的结果表明,目前的双层结构对于制造倾斜的位图案磁记录介质是非常有前途的。

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