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Modeling of Magnetization Distribution Near Shaped Boundary of Garnet Film Core in Fluxgate Magnetometer

机译:磁通门磁力计中石榴石薄膜磁心形边界附近磁化分布的建模

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摘要

Micromagnetic modeling of magnetization in-plane distribution near shaped boundary of garnet film was made to analyze the possibility to prevent chaotic formation of magnetic flux distortions in a fluxgate disc-like core excited by rotating magnetic field. Calculations made in the limit of zero anisotropy for sinusoidal, rectangular, and cogged (with right angle) boundaries show regular macroscopic vortex formation and annihilation in opposite phases of external magnetic field inside every apex of garnet film shaped boundary. Vortices are formed due to magnetostatic conservation of magnetization initial local direction along smooth or straight boundaries of the film during the whole period of rotation. Vortices near smooth curved boundary exhibit a stability range in the external field that exceeds that near rectangular and cogged shapes by an order of magnitude. Transformations of vortex states and low field saturation near broken line boundary are explained by peculiarities of exchange energy caused by mutually perpendicular spin orientations along adjacent straight sides of right angles. Calculation results show the way for control of magnetization distribution distortions in fluxgate garnet disc core by film boundary shape.
机译:建立了石榴石薄膜形状边界附近的磁化面内分布的微磁模型,以分析防止由旋转磁场激发的磁通门盘状磁芯中磁通畸变的混沌形成的可能性。对正弦,矩形和带齿(直角)边界的零各向异性​​极限进行的计算表明,在每个石榴石薄膜状边界的顶部内部,在外部磁场的相反相位中,规则的宏观涡旋形成和an灭。由于在整个旋转期间沿着膜的光滑或笔直边界的磁化初始局部方向的静磁守恒,形成了涡旋。靠近平滑弯曲边界的涡流在外场中的稳定范围比矩形和齿形附近的稳定范围大一个数量级。涡流态的转换和虚线边界附近的低场饱和是由沿直角的相邻直边相互垂直的自旋取向引起的交换能量的特殊性来解释的。计算结果表明了通过薄膜边界形状控制磁通门石榴石圆片磁心分布畸变的方法。

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