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Anomalous enhancement of the sheet carrier density beyond the classic limit on a SrTiO(3) surface
Electrostatic carrier accumulation on an insulating (100) surface of SrTiO(3) by fabricating a field effect transistor with Parylene-C (6 nm)/HfO(2) (20 nm) bilayer gate insulator has revealed a mystifying phenomenon: sheet carrier density [Image: see text] is about 10 times as large as [Image: see...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group
2016
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4865841/ https://www.ncbi.nlm.nih.gov/pubmed/27174141 http://dx.doi.org/10.1038/srep25789 |
Sumario: | Electrostatic carrier accumulation on an insulating (100) surface of SrTiO(3) by fabricating a field effect transistor with Parylene-C (6 nm)/HfO(2) (20 nm) bilayer gate insulator has revealed a mystifying phenomenon: sheet carrier density [Image: see text] is about 10 times as large as [Image: see text] ([Image: see text] is the sheet capacitance of the gate insulator, V(G) is the gate voltage, and e is the elementary charge). The channel is so clean to exhibit small subthreshod swing of 170 mV/decade and large mobility of 11 cm(2)/Vs for [Image: see text] of 1 × 10(14) cm(−2) at room temperature. Since [Image: see text] does not depend on either V(G) nor time duration, [Image: see text] beyond [Image: see text] is solely ascribed to negative charge compressibility of the carriers, which was in general considered as due to exchange interactions among electrons in the small [Image: see text] limit. However, the observed [Image: see text] is too large to be naively understood by the framework. Alternative ideas are proposed in this work. |
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