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Manipulating magnetoelectric energy landscape in multiferroics

Magnetoelectric coupling at room temperature in multiferroic materials, such as BiFeO(3), is one of the leading candidates to develop low-power spintronics and emerging memory technologies. Although extensive research activity has been devoted recently to exploring the physical properties, especiall...

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Detalles Bibliográficos
Autores principales: Huang, Yen-Lin, Nikonov, Dmitri, Addiego, Christopher, Chopdekar, Rajesh V., Prasad, Bhagwati, Zhang, Lei, Chatterjee, Jyotirmoy, Liu, Heng-Jui, Farhan, Alan, Chu, Ying-Hao, Yang, Mengmeng, Ramesh, Maya, Qiu, Zi Qiang, Huey, Bryan D., Lin, Chia-Ching, Gosavi, Tanay, Íñiguez, Jorge, Bokor, Jeffrey, Pan, Xiaoqing, Young, Ian, Martin, Lane W., Ramesh, Ramamoorthy
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7275047/
https://www.ncbi.nlm.nih.gov/pubmed/32504063
http://dx.doi.org/10.1038/s41467-020-16727-2
Descripción
Sumario:Magnetoelectric coupling at room temperature in multiferroic materials, such as BiFeO(3), is one of the leading candidates to develop low-power spintronics and emerging memory technologies. Although extensive research activity has been devoted recently to exploring the physical properties, especially focusing on ferroelectricity and antiferromagnetism in chemically modified BiFeO(3), a concrete understanding of the magnetoelectric coupling is yet to be fulfilled. We have discovered that La substitutions at the Bi-site lead to a progressive increase in the degeneracy of the potential energy landscape of the BiFeO(3) system exemplified by a rotation of the polar axis away from the 〈111〉(pc) towards the 〈112〉(pc) discretion. This is accompanied by corresponding rotation of the antiferromagnetic axis as well, thus maintaining the right-handed vectorial relationship between ferroelectric polarization, antiferromagnetic vector and the Dzyaloshinskii-Moriya vector. As a consequence, La-BiFeO(3) films exhibit a magnetoelectric coupling that is distinctly different from the undoped BiFeO(3) films.