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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(...
Autores principales: | , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group
2015
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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 |
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. |
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