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A study of Barkhausen avalanche statistics through the critical disorder in a ferromagnetic thin film: Experimental investigation and theoretical modeling

机译:通过铁磁薄膜中的严重失调进行的巴克豪森雪崩统计研究:实验研究和理论模型

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摘要

It is well known from theoretical models that a ferromagnetic system should undergo a disorder induced phase transition in its magnetization reversal mode at a critical disorder level R-C, below which, the reversal is characterized by the appearance of the so-called spanning avalanche. The critical regime above R-C is characterized by power-law distributed avalanche sizes and durations, whose exponents determine the universality class to which the magnetic system belongs. The most commonly studied among these is the size-exponent tau, which most theoretical models estimate to be in the range 1.3-1.5. However, experimental determinations of this exponent fall in a much wider interval, between 0.98 and 1.8, well outside the domain of the models. This discrepancy, which is far more common for 2D systems, has not been effectively addressed for more than a decade. In this article, we have determined experimentally the size-exponent 'tau' in 2D Permalloy(Ni80Fe20) thin films by measuring Barkhausen noise through the disorder-induced transition using planar Hall effect. This was compared with our simulations of the random field Ising model, an established nucleation model, with a modification that better represented the experimental condition. Our findings indicated that large 'tau'-values would arise in samples with very low disorder levels well outside the critical regime, where the statistics were non-universal. In such samples, our measured 'tau' increased monotonically with temperature, which indicated a decrease in the effective disorder with temperature according to the nucleation models. This temperature dependence could be understood in the light of an extended Neel-Brown model which we had studied earlier, that had predicted a decrease in the width of switching field distribution with increasing temperature. In this context, we also used micromagnetic simulations, which helped to understand the dependence of coercivity on disorder, a property not predicted correctly by the Ising model.
机译:从理论模型众所周知,铁磁系统应在其磁化反转模式下以临界无序水平R-C进行无序诱导的相变,在该水平以下,反转的特征是出现了所谓的跨越雪崩。 R-C之上的临界状态的特征在于幂律分布的雪崩大小和持续时间,其指数决定了磁系统所属的通用性类别。其中最常研究的是大小指数tau,多数理论模型估计其范围在1.3-1.5之间。但是,该指数的实验确定值落在0.98至1.8之间的更大范围内,远远超出了模型范围。这种差异在2D系统中更为普遍,但是十多年来一直没有得到有效解决。在本文中,我们通过使用平面霍尔效应通过无序感应跃迁测量巴克豪森噪声,通过实验确定了二维坡莫合金(Ni80Fe20)薄膜中尺寸指数“ tau”。将此与我们对随机场Ising模型(已建立的成核模型)的仿真进行了比较,并进行了改进,可以更好地代表实验条件。我们的研究结果表明,在临界水平之外的具有非常低的无序水平的样本中,会出现较大的“ tau”值,而在临界状态下,统计数据是非通用的。在这种样品中,我们测得的“ tau”随温度单调增加,这表明根据成核模型,有效无序随温度降低。可以根据我们之前研究的扩展的Neel-Brown模型来理解这种温度依赖性,该模型预测了随着温度的升高,开关场分布宽度的减小。在这种情况下,我们还使用了微磁模拟,这有助于理解矫顽力对无序性的依赖性,而无序性是伊辛模型无法正确预测的。

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