首页> 外文期刊>Physical Review, B. Condensed Matter >Micromagnetic model of noncollective magnetization reversal in ultrathin magnetic dots with in-plane uniaxial anisotropy - art. no. 174418
【24h】

Micromagnetic model of noncollective magnetization reversal in ultrathin magnetic dots with in-plane uniaxial anisotropy - art. no. 174418

机译:具有面内单轴各向异性的超薄磁点非集体磁化反转的微磁模型-艺术。没有。 174418

获取原文
获取原文并翻译 | 示例
           

摘要

In most magnetic systems the magnetization reversal is nonuniform, and is initiated in a so-called "nucleation volume," whose dimensions are by far smaller than the total system volume. For simplicity reasons magnetization reversal theories are usually based on the assumption that coherent rotation occurs in this "nucleation volume." In this approach, self-dipolar fields and exchange forces are obviously not well described, because in reality the nucleation volume is coupled with the rest of the system. In the case of ultrathin dots with in-plane uniaxial anisotropy, we could take into account dipolar fields and the exchange stiffness explicitly. The approximations used to derive analytical equations were suggested by experimental results on real dots. The model yields the nonuniform micromagnetic configuration of nucleation volumes. It predicts nucleation and reversal field values, as well as the field dependence of the energy barrier to be overcome to reverse the dot at finite temperature. The (negative) reversal field is found to increase with the dot thickness T and the volume magnetization M-s, and to decrease with the material anisotropy K. In the low-thickness limit, the reversal field H-r approaches the Stoner-Wohlfarth reversal field H-a with a law close to 1-H-rH-a similar toM(s)(7/2)A(-3/4)K(-1)T(3/2), where A is the exchange constant. The relevance of the approximations used is discussed and demonstrated by the good agreement found for all predictions between experiment and/or numerical calculations on the one hand and the model on the other hand. [References: 57]
机译:在大多数磁性系统中,磁化反转是不均匀的,并且是在所谓的“成核体积”中引发的,其尺寸远小于总系统体积。为简单起见,磁化反转理论通常基于以下假设:相干旋转发生在此“成核体积”中。用这种方法,显然不能很好地描述自偶极场和交换力,因为实际上成核体积与系统的其余部分耦合。对于具有面内单轴各向异性的超薄点,我们可以明确考虑偶极场和交换刚度。实点上的实验结果表明了用于推导解析方程的近似值。该模型产生成核体积的不均匀微磁配置。它预测了成核和反转场的值,以及在有限温度下要克服的能垒反转点的场依赖性。发现(负)反转场随点厚度T和体积磁化强度Ms增大,而随材料各向异性K减小。在低厚度极限下,反转场Hr接近Stoner-Wohlfarth反转场Ha类似于M(s)(7/2)A(-3/4)K(-1)T(3/2)的接近1- Hr Ha 的定律,其中A是交换常数。一方面通过实验和/或数值计算,另一方面通过模型为所有预测找到了良好的一致性,从而讨论并证明了所用近似的相关性。 [参考:57]

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号