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FePt(BN, X, C)(X = Ag, Re)薄膜的磁性与微观结构

Magnetic Properties and Microstructure of FePt(BN, X, C) (X = Ag, Re) Films.

作者信息

Tsai Jai-Lin, Sun Chun-Yu, Lin Jhih-Hong, Huang Yi-Yuan, Tsai He-Ting

机构信息

Department of Materials Science and Engineering, National Chung Hsing University, Taichung 402, Taiwan.

Instrument Center, The Office of Research & Development, National Chung Hsing University, Taichung 402, Taiwan.

出版信息

Nanomaterials (Basel). 2023 Jan 29;13(3):539. doi: 10.3390/nano13030539.

Abstract

A sputtered FePt(BN, Re, C) film, here boron nitride (BN), was compared to a reference sample FePt(BN, Ag, C). Intrinsically, these films illustrate a high anisotropy field (H) and perpendicular magnetocrystalline anisotropy (K),although the reference sample shows a higher value (H = 69.5 kOe, K = 1.74 × 10 erg/cm) than the FePt(BN, Re, C) film (H = 66.9 kOe, K = 1.46 × 10 erg/cm). However, the small difference in the anisotropy constant (K2/K1) ratio presents a close tendency in the angular dependence of the switching field. Extrinsically, the out-of-plane coercivity for the reference sample is 32 kOe, which is also higher than the FePt(BN, Re, C) film (H = 27 kOe), and both films present lower remanence (Mr/Mr = 0.08~0.12), that is, the index for perpendicular magnetic anisotropy. The higher perpendicular magnetization for both films was due to highly (001) textured FePt films, which was also evidenced by the tight rocking width of 4.1°/3.0° for (001)/(002) X-ray diffraction peaks, respectively, and high-enough ordering degree. The reference sample was measured to have a higher ordering degree (S = 0.84) than FePt(BN, Re, C) (S = 0.63). As a result, the Ag segregant shows stronger ability to promote the ordering of the FePt film; however, the FePt(BN, Re, C) film still has comparable magnetic properties without Ag doping. From the surface and elemental composition analysis, the metallic Re atoms found in the FePt lattice result in a strong spin-orbital coupling between transition metal Fe (3d electron) and heavy metals (Re, Pt) (5d electron) and we conducted high magnetocrystalline anisotropy (K). Above is the explanation that the lower-ordered FePt(BN, Re, C) film still has high-enough Ku and out-of-plane Hc. Regarding the microstructure, both the reference sample and FePt(BN, Re, C) show granular structure and columnar grains, and the respective average grain size and distributions are 6.60 nm (12.5%) and 11.2 nm (15.9%). The average widths of the grain boundaries and the aspect ratio of the columnar grain height are 2.05 nm, 1.00 nm, 2.35 nm, and 1.70 nm, respectively.

摘要

将溅射的FePt(BN, Re, C)薄膜(此处为氮化硼(BN))与参考样品FePt(BN, Ag, C)进行比较。本质上,这些薄膜表现出高各向异性场(H)和垂直磁晶各向异性(K),尽管参考样品显示出比FePt(BN, Re, C)薄膜更高的值(H = 69.5 kOe,K = 1.74×10尔格/厘米)(H = 66.9 kOe,K = 1.46×10尔格/厘米)。然而,各向异性常数(K2/K1)比值的微小差异在开关场的角度依赖性上呈现出相近的趋势。外在地,参考样品的面外矫顽力为32 kOe,也高于FePt(BN, Re, C)薄膜(H = 27 kOe),并且两种薄膜都呈现出较低的剩磁(Mr/Mr = 0.08~0.12),即垂直磁各向异性的指标。两种薄膜较高的垂直磁化归因于高度(001)织构的FePt薄膜,(001)/(002) X射线衍射峰分别具有4.1°/3.0°的紧密摇摆宽度以及足够高的有序度也证明了这一点。测量发现参考样品的有序度(S = 0.84)高于FePt(BN, Re, C)(S = 0.63)。结果,Ag偏析剂显示出更强的促进FePt薄膜有序化的能力;然而,FePt(BN, Re, C)薄膜在未掺杂Ag的情况下仍具有可比的磁性能。从表面和元素组成分析来看,在FePt晶格中发现的金属Re原子导致过渡金属Fe(3d电子)与重金属(Re、Pt)(5d电子)之间产生强烈的自旋 - 轨道耦合,并且我们实现了高磁晶各向异性(K)。以上就是低有序度的FePt(BN, Re, C)薄膜仍具有足够高的Ku和面外Hc的解释。关于微观结构,参考样品和FePt(BN, Re, C)都显示出颗粒结构和柱状晶粒,各自的平均晶粒尺寸和分布分别为6.60纳米(12.5%)和11.2纳米(15.9%)。晶界的平均宽度和柱状晶粒高度的纵横比分别为2.05纳米、1.00纳米、2.35纳米和1.70纳米。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/062b/9919657/bfead25ec1dc/nanomaterials-13-00539-g001a.jpg

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