García Javier, Fernández-Roldán Jose A, González Roque, Méndez Miguel, Bran Cristina, Vega Víctor, González Silvia, Vázquez Manuel, Prida Víctor M
Departamento de Física, Facultad de Ciencias, Universidad de Oviedo, C/Federico García Lorca 18, 33007 Oviedo, Spain.
Instituto de Ciencia de Materiales de Madrid, ICMM-CSIC, Sor Juana Inés de la Cruz 3, 28049 Madrid, Spain.
Nanomaterials (Basel). 2021 Nov 15;11(11):3077. doi: 10.3390/nano11113077.
Magnetic nanomaterials are of great interest due to their potential use in data storage, biotechnology, or spintronic based devices, among others. The control of magnetism at such scale entails complexing the nanostructures by tuning their composition, shape, sizes, or even several of these properties at the same time, in order to search for new phenomena or optimize their performance. An interesting pathway to affect the dynamics of the magnetization reversal in ferromagnetic nanostructures is to introduce geometrical modulations to act as nucleation or pinning centers for the magnetic domain walls. Considering the case of 3D magnetic nanowires, the modulation of the diameter across their length can produce such effect as long as the segment diameter transition is sharp enough. In this work, diameter modulated FeCo ferromagnetic nanowires have been grown into the prepatterned diameter modulated nanopores of anodized AlO membranes. Their morphological and compositional characterization was carried out by electron-based microscopy, while their magnetic behavior has been measured on both the nanowire array as well as for individual bisegmented nanowires after being released from the alumina template. The magnetic hysteresis loops, together with the evaluation of First Order Reversal Curve diagrams, point out that the magnetization reversal of the bisegmented FeCo nanowires is carried out in two steps. These two stages are interpreted by micromagnetic modeling, where a shell of the wide segment reverses its magnetization first, followed by the reversal of its core together with the narrow segment of the nanowire at once.
磁性纳米材料因其在数据存储、生物技术或基于自旋电子学的器件等领域的潜在应用而备受关注。在如此小的尺度上控制磁性需要通过调整纳米结构的组成、形状、尺寸,甚至同时调整其中的几个特性,使纳米结构复合化,以便探索新现象或优化其性能。影响铁磁纳米结构中磁化反转动力学的一个有趣途径是引入几何调制,以充当磁畴壁的成核或钉扎中心。考虑到三维磁性纳米线的情况,只要线段直径过渡足够尖锐,沿其长度方向对直径进行调制就能产生这种效果。在这项工作中,已将直径调制的FeCo铁磁纳米线生长到阳极氧化铝(AlO)膜预先图案化的直径调制纳米孔中。通过基于电子的显微镜对其形态和成分进行了表征,同时在纳米线阵列以及从氧化铝模板中释放出来的单个双段纳米线上测量了它们的磁行为。磁滞回线以及一阶反转曲线图的评估表明,双段FeCo纳米线的磁化反转分两步进行。这两个阶段通过微磁学建模进行了解释,其中宽段的壳层首先反转其磁化方向,随后纳米线的芯部与其窄段一起立即反转。