Cargando…

Metal–insulator-transition engineering by modulation tilt-control in perovskite nickelates for room temperature optical switching

In transition metal perovskites ABO(3), the physical properties are largely driven by the rotations of the BO(6) octahedra, which can be tuned in thin films through strain and dimensionality control. However, both approaches have fundamental and practical limitations due to discrete and indirect var...

Descripción completa

Detalles Bibliográficos
Autores principales: Liao, Zhaoliang, Gauquelin, Nicolas, Green, Robert J., Müller-Caspary, Knut, Lobato, Ivan, Li, Lin, Van Aert, Sandra, Verbeeck, Johan, Huijben, Mark, Grisolia, Mathieu N., Rouco, Victor, El Hage, Ralph, Villegas, Javier E., Mercy, Alain, Bibes, Manuel, Ghosez, Philippe, Sawatzky, George A., Rijnders, Guus, Koster, Gertjan
Formato: Online Artículo Texto
Lenguaje:English
Publicado: National Academy of Sciences 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6156682/
https://www.ncbi.nlm.nih.gov/pubmed/30185557
http://dx.doi.org/10.1073/pnas.1807457115
Descripción
Sumario:In transition metal perovskites ABO(3), the physical properties are largely driven by the rotations of the BO(6) octahedra, which can be tuned in thin films through strain and dimensionality control. However, both approaches have fundamental and practical limitations due to discrete and indirect variations in bond angles, bond lengths, and film symmetry by using commercially available substrates. Here, we introduce modulation tilt control as an approach to tune the ground state of perovskite oxide thin films by acting explicitly on the oxygen octahedra rotation modes—that is, directly on the bond angles. By intercalating the prototype SmNiO(3) target material with a tilt-control layer, we cause the system to change the natural amplitude of a given rotation mode without affecting the interactions. In contrast to strain and dimensionality engineering, our method enables a continuous fine-tuning of the materials’ properties. This is achieved through two independent adjustable parameters: the nature of the tilt-control material (through its symmetry, elastic constants, and oxygen rotation angles), and the relative thicknesses of the target and tilt-control materials. As a result, a magnetic and electronic phase diagram can be obtained, normally only accessible by A-site element substitution, within the single SmNiO(3) compound. With this unique approach, we successfully adjusted the metal–insulator transition (MIT) to room temperature to fulfill the desired conditions for optical switching applications.