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GMI Effect in Thin Amorphous Microwires for Sensors and Tuneable Metamateriales Applications

机译:传感器和可调谐超材料应用中的细非晶微线中的GMI效应

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We present the results on GMI effect in thin microwires at elevated frequencies paying special attention to tailoring the GMI effect and achievement of low hysteretic GMI behavior. We measured magnetic field, H, dependence of real part, Z_1 of the longitudinal wire impedance Z (Z = Z_1 + iZ_2) till 4 GHz in Co-rich microwires. We observed considerable GMI effect at GHz frequencies. General features of these dependences are that the magnetic field of maximum shifts to the higher field region increasing the f. Both ΔZ/Z, and hysteresis loops of nearly-zero Co_(67.1)Fe_(3.8)Ni_(1.4) Si_(14.5)B_(11.5)Mo_(1.7) microwires magnetostrictive exhibit strong sensitivity to the ratio, p, of the metallic nucleus diameter to the total microwire diameter. On the other hand field dependence of the off-diagonal voltage response of nearly zero magnetostriction (λ_s ≈ -3× 10~(-7)) Co_(67.1)Fe_(3.8)Ni_(1.4) Si_(14.5)B_(11.5)Mo_(1.7) with metallic nucleus diameter of 6.0, 7.0 and 8.2 μm exhibits anti-symmetrical shape with almost linear growth within the field range from - H_m to H_m associated with the anisotropy field. Current annealing significantly affects the off-diagonal GMI curves of Co_(67.1)Fe_(3.8)Ni_(1.4) Si_(14.5)B_(11.5)Mo_(1.7) microwires with vanishing magnetostriction constant: under DC current annealing the H_m decreases from 480 A/m in as-cast state to 230 A/m after 5 min annealing with 50 mA current. We found, that if the surface anisotropy is not circumferential, then the magnetization and, consequently, the MI curve Z(H) present hysteresis. This hysteresis can be suppressed by application of sufficiently high DC bias current I_B that creates a circumferential bias field H_B. Applications of thin microwires in tuneable metamaterials are discussed.
机译:我们提出了在高频率下细微线中GMI效应的结果,特别注意调整GMI效应和实现低滞后GMI行为。我们测量了富含钴的微丝中直到4 GHz的磁场H,实部的依赖关系,纵向线阻抗Z的Z_1(Z = Z_1 + iZ_2)。我们在GHz频率下观察到了相当大的GMI效应。这些依赖性的一般特征是最大磁场移向更高的磁场区域,从而增大了f。 Co_(67.1)Fe_(3.8)Ni_(1.4)Si_(14.5)B_(11.5)Mo_(1.7)磁致伸缩微丝的ΔZ/ Z和磁滞回线都几乎为零,对金属的比率p具有很强的敏感性原子核直径到微丝总直径。另一方面,接近零磁致伸缩(λ_s≈-3×10〜(-7))Co_(67.1)Fe_(3.8)Ni_(1.4)Si_(14.5)B_(11.5)的对角电压响应的场相关性金属核直径分别为6.0、7.0和8.2μm的Mo_(1.7)在从-H_m到与各向异性场相关的H_m到H_m的范围内,呈现出几乎线性增长的反对称形状。电流退火显着影响磁致伸缩常数消失的Co_(67.1)Fe_(3.8)Ni_(1.4)Si_(14.5)B_(11.5)Mo_(1.7)微丝的对角GMI曲线:在直流电流退火下,H_m从480降低在50 mA电流下退火5分钟后,铸态状态下的A / m达到230 A / m。我们发现,如果表面各向异性不是圆周各向异性,则磁化强度以及MI曲线Z(H)会出现磁滞现象。可以通过施加足够高的DC偏置电流I_B来抑制此磁滞,该电流会产生圆周偏置磁场H_B。讨论了细微线在可调谐超材料中的应用。

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