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Engineering new limits to magnetostriction through metastability in iron-gallium alloys

Magnetostrictive materials transduce magnetic and mechanical energies and when combined with piezoelectric elements, evoke magnetoelectric transduction for high-sensitivity magnetic field sensors and energy-efficient beyond-CMOS technologies. The dearth of ductile, rare-earth-free materials with hig...

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Detalles Bibliográficos
Autores principales: Meisenheimer, P. B., Steinhardt, R. A., Sung, S. H., Williams, L. D., Zhuang, S., Nowakowski, M. E., Novakov, S., Torunbalci, M. M., Prasad, B., Zollner, C. J., Wang, Z., Dawley, N. M., Schubert, J., Hunter, A. H., Manipatruni, S., Nikonov, D. E., Young, I. A., Chen, L. Q., Bokor, J., Bhave, S. A., Ramesh, R., Hu, J.-M., Kioupakis, E., Hovden, R., Schlom, D. G., Heron, J. T.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8115637/
https://www.ncbi.nlm.nih.gov/pubmed/33980848
http://dx.doi.org/10.1038/s41467-021-22793-x
Descripción
Sumario:Magnetostrictive materials transduce magnetic and mechanical energies and when combined with piezoelectric elements, evoke magnetoelectric transduction for high-sensitivity magnetic field sensors and energy-efficient beyond-CMOS technologies. The dearth of ductile, rare-earth-free materials with high magnetostrictive coefficients motivates the discovery of superior materials. Fe(1−x)Ga(x) alloys are amongst the highest performing rare-earth-free magnetostrictive materials; however, magnetostriction becomes sharply suppressed beyond x = 19% due to the formation of a parasitic ordered intermetallic phase. Here, we harness epitaxy to extend the stability of the BCC Fe(1−x)Ga(x) alloy to gallium compositions as high as x = 30% and in so doing dramatically boost the magnetostriction by as much as 10x relative to the bulk and 2x larger than canonical rare-earth based magnetostrictors. A Fe(1−x)Ga(x) − [Pb(Mg(1/3)Nb(2/3))O(3)](0.7)−[PbTiO(3)](0.3) (PMN-PT) composite magnetoelectric shows robust 90° electrical switching of magnetic anisotropy and a converse magnetoelectric coefficient of 2.0 × 10(−5) s m(−1). When optimally scaled, this high coefficient implies stable switching at ~80 aJ per bit.