Bran Cristina, Fernandez-Roldan Jose Angel, P Del Real Rafael, Asenjo Agustina, Chen Yu-Shen, Zhang Junli, Zhang Xixiang, Fraile Rodríguez Arantxa, Foerster Michael, Aballe Lucia, Chubykalo-Fesenko Oksana, Vazquez Manuel
Instituto de Ciencia de Materiales de Madrid, CSIC, Madrid 28049, Spain.
Department of Physics, University of Oviedo, Oviedo 33007, Spain.
ACS Nano. 2020 Oct 27;14(10):12819-12827. doi: 10.1021/acsnano.0c03579. Epub 2020 Oct 1.
CoNi/Ni multisegmented cylindrical nanowires were synthesized an electrochemical route. The wires are 140 nm in diameter, with 1000 nm long Ni segments and CoNi segments between 600 and 1400 nm in length. The magnetic configuration was imaged by XMCD-PEEM in the demagnetized state and at remanence after magnetizing axially and perpendicularly. Ni segments, with cubic crystal symmetry, show an axial magnetic configuration with a small curling component at the surface. In turn, CoNi segments, with hexagonal crystal symmetry and a strong magnetocrystalline anisotropy perpendicular to the nanowires, show a single vortex state in the shorter segments and multivortex or multitransverse magnetic configurations in medium and long segments, respectively. A detailed study by micromagnetic simulations reveals that the magnetic configuration is determined mainly by the coupling between soft Ni and harder CoNi segments. For short CoNi segments, Ni segments are magnetostatically coupled and the chirality of the single vortex formed in CoNi remains the same as that of the curling in neighboring Ni segments. For longer CoNi segments, the remanent state is either the multivortex or multitransverse state depending on whether the previously applied field was parallel or perpendicular to the magnetocrystalline axis. The results point out the relevance of the cylindrical geometry to promote the occurrence of complex magneto-chiral effects and provide key information for the design of cylindrical magnetic nanowires for multiple applications.
通过电化学方法合成了CoNi/Ni多段圆柱形纳米线。这些纳米线直径为140 nm,具有1000 nm长的Ni段以及长度在600至1400 nm之间的CoNi段。通过XMCD - PEEM对去磁状态以及轴向和垂直磁化后的剩磁状态下的磁结构进行成像。具有立方晶体对称性的Ni段呈现出轴向磁结构,在表面有小的卷曲分量。反过来,具有六方晶体对称性且垂直于纳米线具有强磁晶各向异性的CoNi段,在较短段呈现单涡旋状态,在中段和长段分别呈现多涡旋或多横向磁结构。微磁模拟的详细研究表明,磁结构主要由软Ni段和硬CoNi段之间的耦合决定。对于短的CoNi段,Ni段通过静磁耦合,CoNi中形成的单涡旋的手性与相邻Ni段中的卷曲手性相同。对于较长的CoNi段,剩磁状态是多涡旋还是多横向状态取决于先前施加的场是平行还是垂直于磁晶轴。结果指出了圆柱形几何形状对于促进复杂磁手性效应发生的相关性,并为多种应用的圆柱形磁性纳米线设计提供了关键信息。