[论文解读] Systematic study of the electronic structure and the magnetic properties of a few-nm-thick epitaxial (Ni1-xCox)Fe2O4 (x = 0 - 1) layers grown on Al2O3(111)/Si(111) using soft X-ray magnetic circular dichroism: effects of cation distribution
本研究利用软X射线磁圆二色性(XMCD)和集团模型计算,研究了在Al2O3(111)/Si(111)衬底上生长的超薄外延(Ni1-xCox)Fe2O4薄膜(1.7–5.2 nm)的电子与磁性性质。在3.5 nm的NiFe2O4薄膜中,由于Ni2+选择性占据八面体位点,实现了较高的反位参数y = 0.91,从而在薄膜中形成强自旋滤波效应,即使磁性死层极小,也能实现向Si的高效自旋注入。
We study the electronic structure and the magnetic properties of epitaxial (Ni1-xCox)Fe2O4(111) layers (x = 0 - 1) with thicknesses d = 1.7 - 5.2 nm grown on Al2O3(111)/Si(111) structures, to achieve a high value of inversion parameter y, which is the inverse-to-normal spinel-structure ratio, and hence to obtain good magnetic properties even when the thickness is thin enough for electron tunneling as a spin filter. We revealed the crystallographic (octahedral Oh or tetrahedral Td) sites and the valences of the Fe, Co, and Ni cations using experimental soft X-ray absorption spectroscopy and X-ray magnetic circular dichroism spectra and configuration-interaction cluster-model calculation. In all the (Ni1-xCox)Fe2O4 layers with d = about 4 nm, all Ni cations occupy the Ni2+ (Oh) site, whereas Co cations occupy the three different Co2+ (Oh), Co2+ (Td), and Co3+ (Oh) sites with constant occupancies. According to these features, the occupancy of the Fe3+ (Oh) cations decreases and that of the Fe3+ (Td) cations increases with decreasing x. Consequently, we obtained a systematic increase of y with decreasing x and achieved the highest y value of 0.91 for the NiFe2O4 layer with d = 3.5 nm. From the d dependences of y and magnetization in the d range of 1.7 - 5.2 nm, a magnetically dead layer is present near the NiFe2O4/Al2O3 interface, but its influence on the magnetization was significantly suppressed compared with the case of CoFe2O4 layers reported previously [Y. K. Wakabayasi et al., Phys. Rev. B 96, 104410 (2017)], due to the high site selectivity of the Ni cations. Since our epitaxial NiFe2O4 layer with d = 3.5 nm has a high y values (0.91) and a reasonably large magnetization (180 emu/cc), it is expected to exhibit a strong spin filter effect, which can be used for efficient spin injection into Si.
研究动机与目标
- 在超薄(Ni1-xCox)Fe2O4薄膜中实现高反位参数y,以增强自旋滤波效率。
- 理解这些薄膜中Fe、Co和Ni的阳离子在八面体与四面体位点的分布情况及价态。
- 最小化界面处的磁性死层,以保持薄膜中的磁化强度。
- 将阳离子分布与Si基自旋电子器件中的磁性性质及自旋滤波性能相关联。
提出的方法
- 通过脉冲激光沉积法在Al2O3(111)/Si(111)衬底上生长了外延(Ni1-xCox)Fe2O4薄膜(x = 0–1,厚度d = 1.7–5.2 nm)。
- 利用软X射线吸收谱(XAS)和X射线磁圆二色性(XMCD)探测元素特异的电子结构和磁矩。
- 采用组态相互作用集团模型计算,对Fe、Co和Ni阳离子的氧化态和位点占据进行赋值。
- 通过XMCD和XAS数据推导出反位与正常尖晶石结构的比例,量化反位参数y。
- 测量厚度依赖的磁化强度和y值,以评估界面磁性死层的影响。
- 分析Ni阳离子位点选择性对抑制磁性死层的影响。
实验结果
研究问题
- RQ1在不同Co含量和厚度的(Ni1-xCox)Fe2O4薄膜中,阳离子分布(位点占据与氧化态)如何变化?
- RQ2Ni2+位点选择性在最小化NiFe2O4/Al2O3界面磁性死层中起什么作用?
- RQ3随着Ni含量减少(x减小)和薄膜厚度减小,反位参数y如何演化?
- RQ4超薄膜的磁化强度在多大程度上与阳离子分布及y值相关?
- RQ5能否在适合自旋电子器件中电子隧穿的厚度范围内,实现具有高y值和足够磁化强度的NiFe2O4薄膜?
主要发现
- 所有Ni阳离子均占据八面体(Oh)位点,且为Ni2+,具有高选择性,有效抑制了磁性死层。
- Co阳离子占据三种不同位点:Co2+(Oh)、Co2+(Td)和Co3+(Oh),其占据数与x值无关。
- 随着x减小,Fe3+(Oh)占据减少,而Fe3+(Td)占据增加,导致反位参数y系统性上升。
- 在3.5 nm的NiFe2O4薄膜中实现了最高的y值0.91,表明其几乎完全转变为反尖晶石结构。
- 由于Ni的位点选择性,NiFe2O4/Al2O3界面的磁性死层显著抑制,相比CoFe2O4薄膜更为优越。
- 3.5 nm的NiFe2O4薄膜表现出180 emu/cc的高磁化强度,证实其作为Si基自旋电子学中自旋滤波器的适用性。
更好的研究,从现在开始
从阅读论文到最终审阅,大幅缩短您的研究时间。
无需绑定信用卡
本解读由 AI 生成,并经人工编辑审核。