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Theory of magnetic domain dynamics in uniaxial materials

机译:单轴材料磁畴动力学理论

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We have calculated the total Lagrangian and Rayleigh dissipation functions for an isolated domain of arbitrary cross section in an infinite plate with perpendicular anisotropy. Variation of these functions yields a set of coupled equations describing the motion of the center of mass and the boundaryR(phgr;) (in general noncircular) of the domain. We neglectzdependence and assumedgr;/R≪1where dgr; is the wall ``thickness''. The theory is applicable for applied field variations of arbitrary speed and magnitude. For uniform field pulses, the equations reduce to the Callen‐Josephs theory in the weak‐pulse limit. For pulses >2pgr;Ms/agr;, where agr; is the Gilbert parameter, the behavior again tends to be linear with, generally, a greatly reduced apparent mobility, while in the transition region 2pgr;Msagr;
机译:我们计算了具有垂直各向异性的无限板中任意截面的孤立域的总拉格朗日和瑞利耗散函数。这些函数的变化产生一组耦合方程,描述质心的运动和域的边界R(&phgr;)(通常为非圆)。我们忽略了依赖性并假设&dgr;/R2&pgr;Ms/&agr;,其中 &agr; 是吉尔伯特参数,行为再次趋于线性,通常表观迁移率大大降低,而在过渡区域 2&pgr;Ms&agr;

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