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Tailoring the Two Dimensional Electron Gas at Polar ABO(3)/SrTiO(3) Interfaces for Oxide Electronics

The 2D electron gas at the polar/non-polar oxide interface has become an important platform for several novel oxide electronic devices. In this paper, the transport properties of a wide range of polar perovskite oxide ABO(3)/SrTiO(3) (STO) interfaces, where ABO(3) includes LaAlO(3), PrAlO(3), NdAlO(...

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Detalles Bibliográficos
Autores principales: Li, Changjian, Liu, Zhiqi, Lü, Weiming, Wang, Xiao Renshaw, Annadi, Anil, Huang, Zhen, Zeng, Shengwei, Ariando, Venkatesan, T.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2015
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4549792/
https://www.ncbi.nlm.nih.gov/pubmed/26307382
http://dx.doi.org/10.1038/srep13314
Descripción
Sumario:The 2D electron gas at the polar/non-polar oxide interface has become an important platform for several novel oxide electronic devices. In this paper, the transport properties of a wide range of polar perovskite oxide ABO(3)/SrTiO(3) (STO) interfaces, where ABO(3) includes LaAlO(3), PrAlO(3), NdAlO(3), NdGaO(3) and LaGaO(3) in both crystalline and amorphous forms, were investigated. A robust 4 unit cell (uc) critical thickness for metal insulator transition was observed for crystalline polar layer/STO interface while the critical thickness for amorphous ones was strongly dependent on the B site atom and its oxygen affinity. For the crystalline interfaces, a sharp transition to the metallic state (i.e. polarization catastrophe induced 2D electron gas only) occurs at a growth temperature of 515 °C which corresponds to a critical relative crystallinity of ~70 ± 10% of the LaAlO(3) overlayer. This temperature is generally lower than the metal silicide formation temperature and thus offers a route to integrate oxide heterojunction based devices on silicon.