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具有开放边界的薄随机场铁磁体中的临界巴克豪森雪崩。

The critical Barkhausen avalanches in thin random-field ferromagnets with an open boundary.

作者信息

Tadić Bosiljka, Mijatović Svetislav, Janićević Sanja, Spasojević Djordje, Rodgers Geoff J

机构信息

Department for Theoretical Physics, Jožef Stefan Institute, P.O. Box 3000, SI-1001, Ljubljana, Slovenia.

Complexity Science Hub, Vienna, Austria.

出版信息

Sci Rep. 2019 Apr 19;9(1):6340. doi: 10.1038/s41598-019-42802-w.

DOI:10.1038/s41598-019-42802-w
PMID:31004121
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6474887/
Abstract

The interplay between the critical fluctuations and the sample geometry is investigated numerically using thin random-field ferromagnets exhibiting the field-driven magnetisation reversal on the hysteresis loop. The system is studied along the theoretical critical line in the plane of random-field disorder and thickness. The thickness is varied to consider samples of various geometry between a two-dimensional plane and a complete three-dimensional lattice with an open boundary in the direction of the growing thickness. We perform a multi-fractal analysis of the Barkhausen noise signals and scaling of the critical avalanches of the domain wall motion. Our results reveal that, for sufficiently small thickness, the sample geometry profoundly affects the dynamics by modifying the spectral segments that represent small fluctuations and promoting the time-scale dependent multi-fractality. Meanwhile, the avalanche distributions display two distinct power-law regions, in contrast to those in the two-dimensional limit, and the average avalanche shapes are asymmetric. With increasing thickness, the scaling characteristics and the multi-fractal spectrum in thicker samples gradually approach the hysteresis loop criticality in three-dimensional systems. Thin ferromagnetic films are growing in importance technologically, and our results illustrate some new features of the domain wall dynamics induced by magnetisation reversal in these systems.

摘要

利用在磁滞回线上呈现场驱动磁化反转的薄随机场铁磁体,对临界涨落与样品几何形状之间的相互作用进行了数值研究。该系统是在随机场无序度和厚度平面内沿着理论临界线进行研究的。改变厚度以考虑二维平面和具有沿厚度增长方向开放边界的完整三维晶格之间各种几何形状的样品。我们对巴克豪森噪声信号进行了多重分形分析,并对畴壁运动的临界雪崩进行了标度分析。我们的结果表明,对于足够小的厚度,样品几何形状通过修改代表小涨落的频谱段并促进时间尺度相关的多重分形性,深刻地影响动力学。同时,与二维极限情况相比,雪崩分布显示出两个不同的幂律区域,并且平均雪崩形状是不对称的。随着厚度增加,较厚样品中的标度特性和多重分形谱逐渐接近三维系统中的磁滞回线临界性。薄铁磁膜在技术上的重要性日益增加,我们的结果说明了这些系统中磁化反转引起的畴壁动力学的一些新特征。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dca8/6474887/4de5e21c9695/41598_2019_42802_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dca8/6474887/320d2e469474/41598_2019_42802_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dca8/6474887/071a3a873670/41598_2019_42802_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dca8/6474887/560014dab2ac/41598_2019_42802_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dca8/6474887/b03f0baea091/41598_2019_42802_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dca8/6474887/a60737d3b9f6/41598_2019_42802_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dca8/6474887/932d9b580dd8/41598_2019_42802_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dca8/6474887/17887691aee0/41598_2019_42802_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dca8/6474887/eac9935ee648/41598_2019_42802_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dca8/6474887/4de5e21c9695/41598_2019_42802_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dca8/6474887/320d2e469474/41598_2019_42802_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dca8/6474887/071a3a873670/41598_2019_42802_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dca8/6474887/560014dab2ac/41598_2019_42802_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dca8/6474887/b03f0baea091/41598_2019_42802_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dca8/6474887/a60737d3b9f6/41598_2019_42802_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dca8/6474887/932d9b580dd8/41598_2019_42802_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dca8/6474887/17887691aee0/41598_2019_42802_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dca8/6474887/eac9935ee648/41598_2019_42802_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/dca8/6474887/4de5e21c9695/41598_2019_42802_Fig9_HTML.jpg

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