2012
DOI: 10.1103/physrevb.86.165205
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Physical properties of transparent perovskite oxides (Ba,La)SnO3with high electrical mobility at room temperature

Abstract: Transparent electronic materials are increasingly in demand for a variety of optoelectronic applications, ranging from passive transparent conductive windows to active thin film transistors. suggest that the doped BaSnO 3 system holds great potential for realizing all perovskite-based, transparent high-temperature high-power functional devices as well as highly mobile two-dimensional electron gas via interface control of heterostructured films.

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Cited by 283 publications
(161 citation statements)
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“…The increase in apparent optical gap with La doping is possibly consistent with optical absorption spectra of BaSnO 3 and (Ba,La)SnO 3 obtained by Kim and co-workers, 12 do not show large gaps above the CBM, but instead show other bands within 3 eV of the CBM. These arise from the dimensional reduction, specifically the strongly reduced hopping along the k z , c-axis direction, which narrows the conduction bands.…”
supporting
confidence: 89%
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“…The increase in apparent optical gap with La doping is possibly consistent with optical absorption spectra of BaSnO 3 and (Ba,La)SnO 3 obtained by Kim and co-workers, 12 do not show large gaps above the CBM, but instead show other bands within 3 eV of the CBM. These arise from the dimensional reduction, specifically the strongly reduced hopping along the k z , c-axis direction, which narrows the conduction bands.…”
supporting
confidence: 89%
“…5 This basic result was found in subsequent band structure calculations with various methods. [12][13][14][15][16][17][18][19][20][21][22] Large variation in the band gap between BaSnO 3 , SrSnO 3 , and CaSnO 3 , was found by Mizoguchi and co-workers, 13 and subsequently discussed in terms of strain. 15,17 The band structures with the TB-mBJ potential are shown in Fig.…”
mentioning
confidence: 93%
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“…Note that careful control of the p(O 2 ) is essential for achieving simultaneous increases in the structural and electrical properties, which can explain the further improvement in the RT μ e at the small expense of point defect generation by precise p(O 2 ) control Fig. 4 Comparison of the room temperature electron mobility vs. carrier concentration for our optimized LBSO films wet 0.5% H 2 -annealed at 950°C (red stars) and previously reported LBSO films, i.e., PLD-grown LBSO thin films on an STO substrate 11 (black squares), and on a single-crystal BSO substrate 16 (green circles), MBE-grown LBSO thin films on an STO substrate 13 (blue triangles, orange diamonds), and single-crystal LBSO 38 (pink hexagons)…”
Section: Resultsmentioning
confidence: 99%
“…Owing to this behavior, Sn in II-IV perovskite A 2+ B 4+ O 3 structure can occupy both A-and B-sites, which results in a number of significant synthesis challenges along the route to novel Sn-based perovskite compounds that have recently generated a lot of interest in the functional materials community. SrSnO 3 and BaSnO 3 , with Sn 4+ residing on the B-site, have recently emerged as indium-free transparent conductors [6][7][8] and for oxide electronics due to their high room-temperature electron mobility and wide bandgap. [9][10][11][12][13][14] Mixed valence states may or may not be beneficial, depending on the intended application.…”
Section: © 2016 Author(s) All Article Content Except Where Otherwismentioning
confidence: 99%