V. V. Kuts, A. Turutin, A. Kislyuk, I. Kubasov, E. E. Maksumova, A. A. Temirov, M. D. Malinkovich, N. A. Sobolev, Yuri N. Parkhomenko
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引用次数: 0
摘要
磁电(ME)复合材料具有广泛的应用前景,特别是在磁心动图和磁脑电图医疗诊断设备中作为室温弱磁场传感器。在大多数有关 ME 复合材料的研究中,结构都是在均匀磁场中进行测试的;然而,为了实际应用,有必要详细了解它们在不均匀磁场(IMF)中的行为。在这项工作中,我们测量了交变电流(AC)通过单根细线时产生的径向对称的 IMF,该电流通过 ME 传感器的不同位置。我们创建了一个对磁场灵敏度为 120 V/T 的 ME 自偏压 b-LN/Ni/Metglas 结构,用于 IMF 检测。通过加入具有剩磁化的镍层,避免了外部偏置磁场的必要性。在没有外部直流磁场的情况下,ME 复合材料显示出 0.24 V/(cm - Oe)的非零 ME 系数。研究表明,位于交流 IMF 中的 ME 复合材料的输出电压振幅取决于被研究样品和磁场线的相对位置。当 ME 样品的长边垂直于导线,且将长边分成两个相似部分的对称面包含导线轴线时,可获得最大 ME 信号。在没有振动和其他噪音的情况下,频率范围为 400 Hz 至 1000 Hz,探测极限为 (2 ± 0.4) nT/Hz1/2。
Detection of inhomogeneous magnetic fields using magnetoelectric composites
Magnetoelectric (ME) composites have a wide range of possible applications, especially as room-temperature sensors of weak magnetic fields in magnetocardiography and magnetoencephalography medical diagnostic equipment. In most works on ME composites, structures are tested in uniform magnetic fields; however, for practical application, detailed knowledge of their behaviour in inhomogeneous magnetic fields (IMFs) is necessary. In this work, we measured IMFs with radial symmetry produced by alternate currents (AC) passing through an individual thin wire upon different placements of an ME sensor. An ME self-biased b-LN/Ni/Metglas structure with a sensitivity to the magnetic field of 120 V/T was created for IMF detection. The necessity of an external biasing magnetic field was avoided by the inclusion of a nickel layer having remanent magnetization. The ME composite shows a non-zero ME coefficient of 0.24 V/(cm · Oe) in the absence of an external DC magnetic field. It is shown that the output voltage amplitude from the ME composite, which is located in an AC IMF, is dependent on the relative position of the investigated sample and magnetic field lines. Maximum ME signal is obtained when the long side of the ME sample is perpendicular to the wire, and the symmetry plane which divides the long side into two similar pieces contains the wire axis. In the frequency range from 400 Hz to 1000 Hz in the absence of vibrational and other noises, the detection limit amounts to (2 ± 0.4) nT/Hz1/2.