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Detection of inhomogeneous magnetic fields using magnetoelectric composites
被引:0
|作者:
Kuts V.V.
[1
]
Turutin A.V.
[1
]
Kislyuk A.M.
[1
]
Kubasov I.V.
[1
]
Maksumova E.E.
[1
]
Temirov A.A.
[1
]
Malinkovich M.D.
[1
]
Sobolev N.A.
[1
,2
]
Parkhomenko Y.N.
[1
]
机构:
[1] National University of Science and Technology “MISIS”, 4-1 Leninsky Ave, Moscow
[2] Department of Physics and I3N, University of Aveiro, Aveiro
来源:
Modern Electronic Materials
|
2023年
/
9卷
/
03期
基金:
俄罗斯科学基金会;
关键词:
biasing layer;
bidomain lithium niobate;
composite structures;
inhomogeneous magnetic field;
magnetoelectric effect;
metglas;
nickel;
D O I:
10.3897/j.moem.9.3.114129
中图分类号:
学科分类号:
摘要:
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. © 2023 National University of Science and Technology MISIS.
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页码:105 / 113
页数:8
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