铁基巨磁阻抗薄膜的研究

溅射方法制备的非晶Ｆｅ６８Ｃｕ０．５Ｃｒ４Ｖ５Ｓｉ１３．５Ｂ９薄膜,通过适宜的退火处理得到具有纳米ａ－Ｆｅ（Ｓｉ）和非晶母相的混合结构和最佳的软磁性能,相应的巨磁阻抗值最高可达７２％。本着重研究了热处理条件、薄膜组织结构、较磁性能以及驱动电流频率对Ｆｅ６８Ｃｕ０．５Ｃｒ４Ｓｉ１３．５Ｂ９薄膜磁致阻抗的影响。     

非晶态合金丝巨应力电阻效应的研究

研究了具有近零磁致伸缩系数Ｆｅ４．３５Ｃｏ６８．１５Ｓｉ１２．５Ｂ１５晶态合金丝在外加压应力作用下显示的巨应力电阻抗效应。比较了Ｆｅ４．３５Ｃｏ６８．１５Ｓｉ１２．５Ｂ１５非晶材料及具有大磁致伸缩系数的Ｆｅ７７．５Ｓｉ７．５Ｂ１５非晶材料在弯曲应力作用下显示的应力电阻抗效应的异同。仔细胞研究了结果非晶丝两端的电压信号峰峰值与外力,驱动电流Ｉｍｓ及频率ｆ的     

Fe84Zr7B9薄带中的巨磁阻抗效应

详细研究了Ｆｅ８４Ｚｒ７Ｂ９薄带中的巨磁阻抗效应。研究了退火工艺对巨磁阻抗效应的影响。发现６００℃退火２０ｍｉｎ的Ｆｅ８４Ｚｒ７Ｂ９薄带在１．５ＭＨｚ下的（Ｚｍａｘ（Ｈ）－Ｚ（５２００Ａ／ｍ）／Ｚ（５２００Ａ／ｍ）达到１５２％。同时我们还测量磁导率随磁场的变化关系,研究了不同退火工艺下材料的磁导率,发现材料磁导率值与巨磁阻效应的大小紧密相关。     

低温应力退火Fe基合金薄带巨磁阻抗特性的研究

通过同步辐射X射线衍射技术,观测Fe73.5Cu1Nb3Si13.5B9非晶薄带经过不同温度和不同应力退火60 min后样品的微观结构,利用HP4294A型阻抗分析仪测量相应样品的巨磁阻抗比与磁各向异性。研究结果表明,在450℃下施加不同应力退火的样品仍然处于非晶结构状态,并且在应力为112.1 MPa的条件下产生优异的磁性能,样品的最大巨磁阻抗比达到了1818.7%,是自由退火条件下最大巨磁阻抗比的1.9倍,同时能够改变巨磁阻抗曲线的形状,使Fe基合金薄带的巨磁阻抗曲线具有宽线性的特性。对实验数据进行拟合后发现,样品的最大巨磁阻抗比和磁各向异性场与外加应力都具有线性关系,磁感灵敏度与外加应力具有负指数关系。通过探究发现具有非晶结构的Fe基合金薄带的磁学性能对应力敏感,可以作为研究非晶纳米晶合金材料应力敏感问题的另一个新方向。     

应力作用下电流退火对钴基非晶薄带的巨磁阻抗效应的影响研究

采用应力作用下的直流电流退火处理Co68.2Fe2.3Mo2Si12.5B15非晶薄带，详细讨论了应力退火前后Co基薄带的巨磁阻抗效应的变化，以及退火时间对巨磁阻抗效应的影响，研究表明：应力作用下的电流退火有利于巨磁阻抗效应的提高，并可以通过控制退火时间控制阻抗与外场变化关系曲线形状。     

热处理对F79.5P12C6Cu0.5Mo0.5Si1.5软磁合金薄带的巨磁致阻抗效应

研究了不同温度热处理对Ｆｅ７９．５Ｐ１２Ｃ６Ｃｕ０．５Ｍｏ０．５Ｓｉ１．５的巨磁阻抗的影响，发现ＧＭＩ不仅与磁导率有关，而且也受到磁各向异性的作用。     

热处理对Fe_(79.5)P_(12)C_6Cu_(0.5)Mo_(0.5)Si_(1.5)软磁合金薄带的巨磁致阻抗效应(GMI)的影响

研究了不同温度热处理对Ｆｅ７９．５Ｐ１２Ｃ６Ｃｕ０．５Ｍｏ０．５Ｓｉ１．５的巨磁阻抗的影响，发现ＧＭＩ不仅与磁导率有关，而且也受到磁各向异性的作用。     

软磁薄带巨磁阻抗效应的数值分析

利用磁畴壁移动模型以纳米晶软磁合金Ｆｅ７３．５Ｃｕ１Ｎｂ３Ｓｉ１３．５Ｂ９为例对软磁薄带中的巨磁阻抗效应进行了数值分析，结果发现不同的磁导率机制并不能显著发迹巨巨磁阻抗效的大小仅由磁导率对外加磁场的敏感性决定，从趋肤深度的角度讨论了巨磁阻抗效应的频率特性。     

铁基纳米微晶玻璃包裹丝的软磁性能及巨磁阻抗效应

采用高频感应加热熔融拉引法制备Fe73.0Cu1.0Nb1.5V2.0Si13.5B9.0玻璃包裹合金非晶细丝，经不同温度下退火处理得到玻璃包裹纳米微晶丝，并对其软磁性能及其巨磁阻抗效应的特点进行了研究。结果表明，样品在退火温度为540～570℃时具有最佳软磁性能，并在570℃得到最大磁阻抗变化为253％．是目前国际同类材料的玻璃包裹丝中观察到的最大值。     

同轴电缆结构复合丝巨磁阻抗效应的研究

采用脉冲电沉积工艺在直径为200μm的铜丝表面沉积铁镍合金镀层,形成具有同轴电缆结构的巨磁阻抗复合丝材料。分别改变复合丝磁性外壳厚度与铜丝直径,研究复合丝结构对巨磁阻抗效应的影响。发现巨磁阻抗比值随磁性外壳厚度的增大及铜丝直径的增大而增大,特征频率则向低频端移动。本文还发现在外加直流磁场低于5．57kA／m时,驱动交流电幅值增大,巨磁阻抗效应增大;高于5．57kA／m时,驱动交流电幅值的大小几乎不再影响复合丝的巨磁阻抗效应。在驱动电流上叠加20mA以下的直流偏置对巨磁阻抗效应没有影响。     

高磷含量CoP-Cu复合丝巨磁阻抗效应的频谱特性

控制电化学工艺条件在直径为200μm的铜丝表面合成CoP磁性镀层成功地制备出高磷含量CoP—Cu复合丝巨磁阻抗效应材料。当磷含量为20%（原子分数）时,复合丝巨磁阻抗效应非常显著,达80%以上。本文详细研究了复合丝材料的频谱及巨磁阻抗效应频谱,指出复合丝巨磁阻抗具有较低的特征频率及较宽的频率使用范围与此新型结构有关,本文还发现,随频率的增加,最大负巨磁阻抗比对应的外加直流磁场也在增加,并且在高频与低频时,巨磁阻抗效应随磁场的响应曲线明显不同。     

电流退火对CoFeSiB非晶丝和薄带的巨磁阻抗效应比较

采用熔融抽拉法和单辊急冷法分别制备了Co68.25Fe4.5Si12.25B15非晶丝和薄带。测量了制备态下两者的巨磁阻抗(GMI)效应,发现非晶丝的GMI比率高于薄带。研究了不同电流密度退火后非晶丝和薄带的GMI效应,结果发现ΔΖ/Ζ=[Z(H)-Z(H=0)]/Z(H=0)都明显上升,且非晶薄带数值更大;当电流密度等于0.96×107A/m2时,薄带的这一比率最大达到410%,磁场灵敏度达到5.1%/(A/m)。分析了出现上述现象的原因。     

GMI磁传感器内部灵敏度与噪声特性研究

建立了非晶带GMI敏感元件的灵敏度和噪声理论模型,计算了其灵敏度和磁噪声在不同易轴方向和外磁场应用条件下的响应特性.通过改变易轴方向、外磁场及直流偏置场对非晶带敏感元件进行了优化,其内部磁噪声达到了fT/(√HZ)水平.分析了内部灵敏度、工作点和磁噪声水平对GMI磁传感器性能的影响,结果表明,在GMI磁传感器设计时,应...     

巨磁阻抗传感器敏感材料的选择

利用巨磁阻抗(GMI)效应来研制传感器,敏感材料的选择非常关键,其GMI性能的好坏直接决定了GMI磁传感器的灵敏度水平.讨论了GMI材料的选择标准,列出了能够产生GMI效应的各种材料,并分析和评述了这些GMI材料的软磁特性、GMI效应及其在传感器上的可能应用,提供了设计高性能GMI传感器的候选材料,这些材料以及新型材料的开发为GMl传感器的研制创造了有利的条件,将会促进GMI传感器的发展与应用.     

Equivalent Magnetic Noise Limit of Low-Cost GMI Magnetometer

We present a noise analysis of a giant magnetoimpedance (GMI) sensor using a peak detector at the optimal magnetic field working bias point of a sensor wire, by considering internal noise sources (intrinsic GMI device associated noise sources and conditioning electronic noise sources). An expression is obtained for the theoretical expected noise for known electronic design parameters and physical characteristics of the GMI wire. The most significant contributions to noise in a GMI measurement, using two basic oscillators (either a simple discrete RC oscillator or quartz oscillator) along with a peak detector, are presented. We discuss the expected extrinsic equivalent magnetic noise limit.      

The effect of magnetic field orientation on the magnetoimpedance of electroplated NiFeCo/Cu wire

Journal of Materials Science: Materials in Electronics - Giant magnetoimpedance (GMI) effect in electrodeposited NiFeCo/Cu wire is studied in the intermediate frequency region...     

Dependence of frequency and amplitude of the ac current on the GMI properties of Co based amorphous wires

The frequency and the amplitude of the driving ac current dependence of the Giant Magneto-Impedance (GMI) behaviour in (Fe₆Co₉₄)_72.5Si_12.5B₁₅ amorphous wire have been studied. The single and two-peak behaviour in the GMI characteristics are observed which depends on the amplitude and frequency of the ac driving current flowing through the sample. The GMI ratio initially increased and then decreased monotonically with the increase of frequency, f, and the amplitude of the ac current, I_ac. With the increase of amplitude of ac current, the response of the GMI voltage is found non-linear with the generation of higher harmonics. With the increase of higher harmonics, the first harmonic component of the GMI voltage started decreasing. With the increase of the ac current, the field sensitivity of the first harmonic components of the GMI voltage decreases and in higher harmonics it shows an increasing trend. The maximum field sensitivity was observed 7.5% per A/m for I_ac = 2 mA and at frequency 100 kHz. The paper investigates the response of the second and third harmonics with the frequencies and amplitude of the driving current. A voltage equation derived from the rotational model to study the response of the GMI voltage.     

Giant Magnetoimpedance Effect: Concept and Prediction in Amorphous Materials

Giant magneto impedance (GMI) effect was experimentally measured on as-cast, post-production and coated with chemical technique amorphous wire and ribbon materials consisted of varied chemical composition over a frequency range from 0.1 to 8 MHz under a static magnetic field between ?8 and +8 kA/m. The results show that each amorphous sample has a certain operational frequency for which the GMI effect has maximum magnitude and the other parameters such as annealing and coating have a significant influence on the GMI effect. It is believed that the domain structure and wall mechanism in the material are responsible for this behaviour. A 3-node input layer, 1-node output layer artificial neural network (ANN) model with three hidden layers including 30 neurons and full connectivity between the nodes was developed. A total of 1600 input vectors obtained from varied treated samples was available in the training data set. After the network was trained, better results were obtained from the network formed by the hyperbolic tangent transfer function in the hidden layers, there was a sigmoid transfer function in the output layer and we predicted the GMI. Comparing the predicted values obtained from the ANN model with the experimental data indicates that a well-trained neural network model provides very accurate results.     

三明治结构FeNi/Cu/FeNi多层膜巨磁阻抗效应研究

采用MEMS技术在玻璃基片上制备了三明治结构FeNi/Cu/FeNi多层膜,在1～40 MHz范围内研究了FeNi/Cu/FeNi多层膜中的巨磁阻抗效应特性.当磁场Ha施加在薄膜的长方向时,巨磁阻抗效应随磁场的增加而增加,在某一磁场下达到最大值,然后随磁场的增加而下降到负的巨磁阻抗效应.在频率为5MHz时,巨磁阻抗效应在磁场Ha=800 A/m时达到最大值26.6%.巨磁阻抗效应的最大值及负的巨磁阻抗效应与多层膜中磁各向异性轴的取向及发散有关.另外,当磁场施加在薄膜的短方向时,薄膜表现出负的巨磁阻抗效应,在频率5 MHz、磁场Ha=9600 A/m时,巨磁阻抗效应可达-15.6%.