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Fe_(84)Zr_(2.08)Nb_(1.92)Cu_1B_(11)纳米晶薄带中的巨磁阻抗效应 被引量:3

Giant Magneto-Impedance Effect of Fe_(84)Zr_(2.08)Nb_(1.92)Cu_1B_(11)Nanocrystalline Ribbons
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摘要 利用真空甩带机制备了Fe84Zr2.08Nb1.92Cu1B11金属快淬薄带。X射线衍射结果表明:薄带经570℃退火后析出纳米化结构bcca-Fe相,晶粒大小约为20nm^40nm,利用HP4294A阻抗分析仪测量了此纳米晶薄带中的巨磁阻抗效应。结果显示在低频下阻抗随外磁场单调减小,这主要是由于磁导率随外磁场的变化导致的,高频下阻抗随外磁场变化出现1个峰值,这主要是由于横向各向异性的原因。运用计算机模拟了这一结果,发现磁导率随外磁场的变化在外场与各向异性场的比值约为0.9处出现了峰值,巨磁阻抗效应也在此位置出现峰值。并且随着驱动电流频率的增大峰值变大。 The giant magneto-impedance effect of Fe84Zr2.08Nb1.92Cu1B11 ribbons was investigated. The ribbon Fe84Zr2.08Nb1.92Cu1B11 was prepared by melt-spun with a Cu roller speed of 40 m/s. The result of X- ray diffraction shows that the ribbons after being annealed at 570degreesC for 20 min precipitates bcc a-Fe phase with grain size of 20 nmsimilar to40 nm. The magnetoimpedance effect was measured by a HP4194A impedance analyzer at room temperature. The impedance decreases with magnetic field monotonically at low frequency due to the decrease of permeability. At high frequency, the impedance shows a peak, which is due to the transverse anisotropy. Results of model-simulation show that when the ratio of magnetic field to transverse anisotropy field reaches about 0.9. the transverse permeability as well as the impedance undergoes. a peak respectively. For frequencies range of f less than or equal to 10 MHz, the impedance peak-value increases with the increase of frequency.
出处 《稀有金属材料与工程》 SCIE EI CAS CSCD 北大核心 2005年第1期120-123,共4页 Rare Metal Materials and Engineering
基金 国家自然科学基金资助(资助号50271036)
关键词 纳米晶薄带 巨磁阻抗效应 磁导率 nanocrystalline ribbon giant magnetoimpedance permeability
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