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首页> 外文期刊>Physical Review, B. Condensed Matter >Random and exchange anisotropy in consolidated nanostructured Fe and Ni: Role of grain size and trace oxides on the magnetic properties
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Random and exchange anisotropy in consolidated nanostructured Fe and Ni: Role of grain size and trace oxides on the magnetic properties

机译:固结纳米结构铁和镍中的随机和交换各向异性:晶粒尺寸和微量氧化物对磁性的影响

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Results of magnetization measurements on nanocrystalline Fe and Ni produced by inert-gas condensation are presented. The grain size, which is about 10 to 20 nm in the as-prepared state, is increased by annealing the samples incrementally from 100 degrees C to 1000 degrees C. The coercive field shows a pronounced variation with grain size, with a maximum at around 30 nm and a steep decrease for smaller grain sizes. The coercivity is discussed on the basis of the random-anisotropy model that predicts that the effective anisotropy constant is reduced by averaging over magnetically coupled grains. This behavior is observed as long as the grain size is smaller than the effective bulk domain-wall width. The model also accounts for the approach to saturation in nanostructured Fe yielding values for the ferromagnetic correlation length and the anisotropy constant of the grains. The latter is about four times higher than the bulk value of Fe. Hysteresis measurements at 5 K after field cooling show a shift and broadening of the hysteresis loops for both Fe and Ni, which is attributed to an exchange coupling between the ferromagnetic grains and antiferromagnetic or ferrimagnetic (oxide) interfacial phases. The hysteresis shift decreases and finally vanishes with increasing grain size. This is indicative of a restructuring of the oxides, which is confirmed by the coercive field of the Fe samples showing a step at about 120 K caused by a phase transition of Fe,Oa. The step vanishes again with further increasing grain size. The saturation magnetization of the Ni samples increases with increasing annealing temperature, a fact that is attributed to the evolution of the oxides also. [References: 50]
机译:给出了通过惰性气体冷凝产生的纳米晶Fe和Ni的磁化测量结果。通过将样品从100摄氏度逐步升高到1000摄氏度进行逐步退火,晶粒尺寸在准备好的状态下大约为10到20 nm。矫顽场显示出明显的晶粒尺寸变化,最大值出现在周围。 30 nm,并且对于较小的晶粒尺寸会急剧减小。矫顽力是在随机各向异性模型的基础上讨论的,该模型预测通过对磁耦合晶粒进行平均可以降低有效各向异性常数。只要晶粒尺寸小于有效的体畴壁宽度,就可以观察到这种行为。该模型还考虑了铁结构相关长度和晶粒各向异性常数的纳米结构铁屈服值的饱和方法。后者比铁的体积值高约四倍。磁场冷却后在5 K处的磁滞测量结果显示,Fe和Ni的磁滞回线都发生了移动和变宽,这归因于铁磁性晶粒与反铁磁性或亚铁磁性(氧化物)界面相之间的交换耦合。磁滞位移减小,最终随着晶粒尺寸的增大而消失。这表明了氧化物的重组,这已通过Fe样品的矫顽场得到证实,该样品的矫顽场显示了Fe,Oa的相变导致在约120 K处出现台阶。随着晶粒尺寸的进一步增加,该台阶再次消失。 Ni样品的饱和磁化强度随退火温度的升高而增加,这也归因于氧化物的析出。 [参考:50]

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