Effect of N₂ Addition on Nanostructure and Magnetic Properties of Sputtered FePt-BN Granular Films During Deposition for Heat Assisted Magnetic Recording

符号 物理 数学 算术
作者
Kim Kong Tham,Takashi Saito,Ryosuke Kushibiki,Shin Saito
出处
期刊:IEEE Transactions on Magnetics [IEEE Magnetics Society]
卷期号:58 (8): 1-4 被引量:7
标识
DOI:10.1109/tmag.2022.3146934
摘要

Magnetic properties and nanostructure for FePt-30 vol% BN granular films deposited while flowing N 2 gas with ratio between 0% and 5% with respect to the total flow of N 2 + Ar are investigated. Here is a list of the results: 1) A maximum coercivity ( $H_{\mathrm {c}}$ ) of 18.9 kOe, a saturation magnetization ( $M_{\mathrm {s}}$ ) of 600 emu/cm 3 , a perpendicular magnetic anisotropy ( $K_{\mathrm {u\bot }}$ ) of $1.7\times 10^{\mathrm {7}}$ erg/cm 3 , and a magnetic anisotropy field ( $H_{\mathrm {k}}$ ) of 58 kOe, with smaller grain size and higher degree of grain separation are obtained when N 2 gas with a ratio of around 2% is added; 2) higher fraction of N 2 gas ratio leads to an increase of the amount of magnetic grains with $c$ -axis parallel to the film plane; 3) lattice constant $a$ remains constant, a minimum value of lattice constant $c$ and the ratio $c/a$ are also observed for a N 2 ratio of around 2%; 4) there are two phenomena observed in nanostructure and magnetic properties defined by the N 2 ratio. For N 2 ratios under 2%, changes in the $c/a$ ratio, the degree of order, and the agglomeration suppression of grains enhance $M_{\mathrm {s}}$ , $K_{\mathrm {u\bot }}$ , and $H_{\mathrm {k}}$ . This indicates that the segregation of B into grain boundaries as the result of the N 2 addition. For N 2 ratios over 2%, the change of tetragonal into cubic FePt magnetic grains, the reduction of the degree of order, and the decrease of $M_{\mathrm {s}}$ and $K_{\mathrm {u\bot }}$ suggest that excess nitrogen dissolves into the FePt magnetic grains; and 5) another consequence of the 2% N 2 ratio is the enhancement of the magnetic grain decoupling along with the increase of $H_{\mathrm {k}}$ , this results in the maximization of $H_{\mathrm {c}}$ .
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