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Temperature and thickness dependence at the onset of perpendicular magnetic anisotropy in FePd thin films sputtered on MgO(001)

机译:MgO(001)上溅射的FePd薄膜在垂直磁各向异性开始时的温度和厚度依赖性

摘要

The onset of chemical order (L10 phase) and perpendicular magnetic anisotropy in FePd(001) thin films sputtered on MgO(001) at temperatures from room temperature to 700 °C and thickness between 1.4 and 22 nm are investigated. It is found that the formation of the FePd ordered phase exhibiting high perpendicular magnetic anisotropy (L10 phase with the c axis in the growth direction) is affected by a two-dimensional to three-dimensional growth mode transition with increasing deposition temperatures, hindering higher chemical ordering at moderate and high temperatures. For 22-nm-thick films, the ordered phase is only obtained in a narrow range of growth temperature centered at 450 °C. This fact, together with strong surface morphology dependence on the deposition temperature, determines the magnetic and magneto-optical properties of the studied system. No dependence of the ordering degree on film thickness is found for films with thicknesses of 3, 7 and 22 nm grown at 450 °C, with a constant value indicating that chemical ordering occurs since the early stages of growth and does not improve as the growth proceeds. The samples consist of chemically ordered nanostructures that range in size from 30 to 200 nm average diameter and 0.5–30 nm height as the film becomes thicker, and exhibit perpendicular magnetic anisotropy indicating that the c axis is parallel to the direction of growth. The largest coercive field (7 kOe) corresponds to the sample with nano-sized particles, and the coercivity drastically decreases down to 1 kOe as percolation sets in.
机译:研究了从室温到700°C且厚度在1.4到22 nm之间溅射在MgO(001)上的FePd(001)薄膜中化学级(L10相)的发生和垂直磁各向异性。发现具有高垂直磁各向异性的FePd有序相的形成(生长方向为c轴的L10相)受沉积温度升高的二维至三维生长模式转变的影响,从而阻碍了更高的化学反应在中等和高温下订购。对于22 nm厚的薄膜,只有在以450°C为中心的狭窄生长温度范围内才能获得有序相。这一事实,加上对沉积温度的强烈表面形态依赖性,决定了所研究系统的磁和磁光特性。对于在450°C下生长的厚度分别为3、7和22 nm的膜,没有发现有序度对膜厚的依赖性,其恒定值表示从生长的早期开始就发生了化学有序性,并且随着生长的进行而不会改善收益。样品由化学有序的纳米结构组成,随着膜的变厚,纳米结构的尺寸范围为平均直径30至200 nm,高度0.5至30 nm,并表现出垂直的磁各向异性,表明c轴平行于生长方向。最大矫顽场(7 kOe)对应于具有纳米尺寸颗粒的样品,并且随着渗流的开始,矫顽力急剧下降至1 kOe。

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