Abstract

Magnetoelectric (ME) sensors for the weak magnetic field measurement have attracted a lot of attention because of their high sensitivity and easy integration. However, the ME sensor performs well only at its working-point under a direct current (DC) bias field (Hbias) and mechanical resonance frequency (fres). The measurement of DC to ultralow frequency (0–100 Hz) weak magnetic fields has increasing demands, such as in geomagnetic anomaly fields, geological and mineral exploration, magnetocardiography, and magnetoencephalography. Unfortunately, fres of ME sensors is on the order of several tens of kilohertz, which is far higher than the ultralow frequency desired. Moreover, if the operation frequency deviates from fres, the sensitivity will deteriorate rapidly. In this study, a working-point perturbation method was used to measure the weak magnetic fields at 0–100 Hz with a high magnetic field resolution. (1) The perturbation of fres using an ultralow frequency (fac) magnetic field results in two modulation peaks with frequencies of fres ± fac. The frequency and resolution of the measured alternating current magnetic field can be obtained by varying fac and the modulation depth. A resolution around 1 nT for fac > 10 Hz and a lowest operation frequency of 0.1 Hz were achieved using our measurement system. (2) A high field resolution of 3 nT (better than the frequency perturbation method with a resolution of 16 nT at 0.1 Hz) can be achieved by the perturbation of Hbias at fres because the ME sensor is still working at the quasi-working-point and helped by lock-in amplifier technology.

Highlights

  • The magnetoelectric coupling (ME) effect refers to the coupling between magnetization M and electric polarization P

  • Magnetoelectric (ME) sensors for the weak magnetic field measurement have attracted a lot of attention because of their high sensitivity and easy integration

  • superconducting quantum interference device magnetometer (SQUID), atomic magnetometer (AMM), and flux-gate meter (FGM) have high sensitivity; they are flux-type sensors and are very sensitive to the magnetic flux through the sensors

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Summary

Introduction

The magnetoelectric coupling (ME) effect refers to the coupling between magnetization M and electric polarization P The former represents the magnetic properties of the medium, and the latter represents the dielectric properties. SQUID, AMM, and FGM have high sensitivity; they are flux-type sensors and are very sensitive to the magnetic flux through the sensors Their sensitivity decreases rapidly with the decrease in the sensor dimension. ME sensors can be made by thin film technologies and combined with MEMS technologies to realize sensor arrays.10–20 These further meet the requirements of miniaturization and automation for sensors. Their ultralow frequency (f < 100 Hz) and even direct current (DC) magnetic field sensing are of concern. It is very difficult to measure ultralow frequency weak magnetic fields directly with ME sensors and necessary to explore novel measurement methods

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