2013
DOI: 10.1038/ncomms2804
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Anisotropic two-dimensional electron gas at the LaAlO3/SrTiO3 (110) interface

Abstract: The observation of a high-mobility two-dimensional electron gas between two insulating complex oxides, especially LaAlO3/SrTiO3, has enhanced the potential of oxides for electronics. The occurrence of this conductivity is believed to be driven by polarization discontinuity, leading to an electronic reconstruction. In this scenario, the crystal orientation has an important role and no conductivity would be expected, for example, for the interface between LaAlO3 and (110)-oriented SrTiO3, which should not have a… Show more

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Cited by 110 publications
(135 citation statements)
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“…Our results explain the dopant-dependent anisotropy at the (110)-oriented LaAlO 3 /SrTiO 3 interface that was observed recently (22). Although both d xy -and d yz =d zx -derived Fermi surfaces are strongly anisotropic, the difference along the [001] and ½110 directions themselves is not very pronounced at higher carrier density, when both ellipsoids are occupied (Fig.…”
Section: Resultssupporting
confidence: 68%
“…Our results explain the dopant-dependent anisotropy at the (110)-oriented LaAlO 3 /SrTiO 3 interface that was observed recently (22). Although both d xy -and d yz =d zx -derived Fermi surfaces are strongly anisotropic, the difference along the [001] and ½110 directions themselves is not very pronounced at higher carrier density, when both ellipsoids are occupied (Fig.…”
Section: Resultssupporting
confidence: 68%
“…Recently, at (110) orientated LAO/STO interfaces, unexpected high mobility metallic conductivity was also found. 17,18 The quasi 2DEG of the (110) LAO/STO interfaces has similar values of the sheet carrier density, room temperature resistivity and electronic mobility to those found at the (001) LAO/STO interfaces. In addition, a unified mechanism of the origin of the 2DEG for both (001) and (110) LAO/STO interfaces has been proposed.…”
Section: Introductionmentioning
confidence: 56%
“…Some attempts in these directions include the growth of LaAlO 3 /EuTiO 3 /SrTiO 3 [87], showing low T ferromagnetism and 2D-conductivity, LaTiO 3 /LaCrO 3 /SrTiO 3 systems [88], the deposition of ferromagnetic polar layer on STO and other oxides, or the use of other 3d 0 materials like KTaO 3 . Similarly, the atomic control achieved in the growth of these oxides has now provided ways to realize heterostructures where polar discontinuity can be engineered and modified using (110) and (111) interfaces [89,90]. In the latter case, theoretical papers have suggested interesting topological protected states with some analogies with topological insulators [91].…”
Section: Discussion and Concluding Remarksmentioning
confidence: 99%