arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 2603.03477physics.optics
收藏

立方磁化贡献对镍(001)和镍(111)薄膜的磁光 Kerr 效应的影响研究

Cubic-in-magnetization contributions to the magneto-optic Kerr effect investigated for Ni(001) and Ni(111) thin films

VSB-Technical University of Ostrava(俄斯特拉发理工大学);Bielefeld University(比勒费尔德大学);Charles University(查理大学);Czech Technical University(捷克理工大学);Johannes Gutenberg University Mainz(美因茨约翰内斯古腾堡大学)

Robin Silber, Maik Gaerner, Kamil Postava, Jaroslav Hamrle, Timo Kuschel

AI总结:

本文研究了镍(001)和(111)薄膜中立方磁化对磁光Kerr效应的影响,通过理论和实验分析了不同晶向的CMOKE强度及各向异性特性。

摘要:

本文介绍了立方磁化磁光 Kerr 效应(CMOKE)的详细理论,通过推导磁光张量的三阶磁化张量,记为 H,比较不同晶向的 CMOKE 强度的理论和实验结果。在具有立方对称性的晶体中,张量 H 由两个独立参数 H₁₂₃ 和 H₁₂₅ 描述。与线性磁光张量 K 和二次磁光张量 G 一起,介电张量在磁化三阶范围内被描述。我们解析地描述了 MOKE 的方程,包括 QMOKE 和 CMOKE 自身的贡献,分别针对 (001) 和 (111) 倾向的立方晶体结构。这些结果与实验测量的两个样本进行比较,这两个样本分别具有 (001) 和 (111) 倾向的 fcc 镍层。此外,我们使用 Yeh 的 4×4 转移矩阵学说,从介电张量到三阶磁化张量进行模拟和描述。我们发现,源自磁光张量 H 的 MOKE 各向异性,即 ΔH = H₁₂₃ - 3H₁₂₅,对于 (111) 倾向的立方晶体结构更为显著,其表现为 MOKE 的三重平面角依赖性,分别与纵向和横向磁化方向相关。

英文摘要:

*The abstract of this article is too long to be included in the arXiv metadata; please see the paper for the full abstract.* ...In this paper, we introduce the detailed theory of cubic-in-magnetization magneto-optic Kerr effect (CMOKE) by deriving the magneto-optic tensor of third order in magnetization, denoted as $\bm{H}$, and comparing the strength of CMOKE for different crystal orientations theoretically and experimentally. In crystals with cubic symmetry, the tensor $\bm{H}$ is described by two independent parameters $H_{123}$ and $H_{125}$. Together with the linear magneto-optic tensor $\bm{K}$ and quadratic magento-optic tensor $\bm{G}$, the permittivity tensor is described up to third order in magnetization. We analytically describe equations of the MOKE including the contribution of QMOKE and CMOKE itself for (001)- and (111)-oriented cubic crystal structures. Those are compared to experimental measurements of two samples with an (001)- and (111)-oriented fcc Ni layer, respectively. Further, we use Yeh's 4$\times$4 transfer matrix calculus to simulate and describe the experimental measurements phenomenologically from the permittivity tensor up to third order in $\bm{M}$. We find that the MOKE anisotropy that stems from the magneto-optic tensor $\bm{H}$ described as $ΔH = H_{123}-3H_{125}$, is much more pronounced for the (111)-oriented cubic crystal structure, for which it manifests as three-fold in-plane angular dependencies of MOKE with longitudinal and also with transversal magnetization direction, respectively.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

↑