Equivalent Magnetic Noise in Magnetoelectric Laminates Comprising Bidomain LiNbO3 Crystals

JV Vidal, AV Turutin, IV Kubasov… - IEEE Transactions …, 2017 - ieeexplore.ieee.org
JV Vidal, AV Turutin, IV Kubasov, MD Malinkovich, YN Parkhomenko, SP Kobeleva…
IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency …, 2017ieeexplore.ieee.org
The anisotropic direct magnetoelectric (ME) properties of bilayered composites comprising
magnetostrictive metglas foils and single-crystalline piezoelectric bidomain plates of 127° Y-
cut LiNbO 3 (LNO) have been studied theoretically and experimentally. The LNO plates
possessed an engineered ferroelectric macrobidomain structure with opposite spontaneous
polarization vectors. Impedance, ME effect, and equivalent magnetic noise density (EMND)
measurements have been performed under quasi-static and resonant conditions. Whereas …
The anisotropic direct magnetoelectric (ME) properties of bilayered composites comprising magnetostrictive metglas foils and single-crystalline piezoelectric bidomain plates of 127°Y-cut LiNbO 3 (LNO) have been studied theoretically and experimentally. The LNO plates possessed an engineered ferroelectric macrobidomain structure with opposite spontaneous polarization vectors. Impedance, ME effect, and equivalent magnetic noise density (EMND) measurements have been performed under quasi-static and resonant conditions. Whereas the quasistatic ME effect was only two times stronger in the bidomain samples compared to their unidomain and bonded bimorph counterparts, in the bending resonance mode, the effect was up to one order of magnitude stronger: ME coefficients of up to 578 V/(cm · Oe) were obtained at ca. 30 kHz under resonance using 0.5-mm-thick crystals. EMND measurements yielded values down to 153 pT/Hz 1/2 at 1 kHz and 524 fT/Hz 1/2 under resonant conditions. A further optimization of the fabrication techniques, laminate geometry, and detection circuit is expected to allow reducing these values down to at least 10 pT/Hz 1/2 and 250 fT/Hz 1/2 , respectively, and the resonance frequency by at least two orders of magnitude. Such systems may thus find use in simple and sensitive, passive and stable, low frequency and high-temperature vector magnetic field sensors.
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