2012
DOI: 10.1103/physrevx.2.039901
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Erratum: Carrier-Controlled Ferromagnetism inSrTiO3[Phys. Rev. X2, 021014 (2012)]

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Cited by 44 publications
(57 citation statements)
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“…Early evidence suggests that the entrance into a superconducting state is a Berezinskii-KosterlitzThouless transition [8]. At even higher densities, a ferromagnetic phase appears to exist [9,10] and may even coexist with superconductivity [11][12][13].The handful of experiments on the quantum transport properties of two-dimensional electrons in STO have thus far focused on locally patterned LAO/STO, and have produced several interesting observations. The Rashba spin-orbit interaction -extracted from weak antilocalization measurements -is relatively large and tunable by application of a gate voltage.…”
mentioning
confidence: 99%
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“…Early evidence suggests that the entrance into a superconducting state is a Berezinskii-KosterlitzThouless transition [8]. At even higher densities, a ferromagnetic phase appears to exist [9,10] and may even coexist with superconductivity [11][12][13].The handful of experiments on the quantum transport properties of two-dimensional electrons in STO have thus far focused on locally patterned LAO/STO, and have produced several interesting observations. The Rashba spin-orbit interaction -extracted from weak antilocalization measurements -is relatively large and tunable by application of a gate voltage.…”
mentioning
confidence: 99%
“…Early evidence suggests that the entrance into a superconducting state is a Berezinskii-KosterlitzThouless transition [8]. At even higher densities, a ferromagnetic phase appears to exist [9,10] and may even coexist with superconductivity [11][12][13].…”
mentioning
confidence: 99%
“…[1][2][3][4][5][6] While a large number of perovskite based heterostructures have been discovered experimentally so far [7][8][9][10][11][12][13][14] , all of these systems contain layers of quantum paraelectric SrTiO 3 (STO) 15 except for the notable LaTiO 3 /KTaO 3 14 . Among these STO-based systems, specifically for the RTiO 3 /SrTiO 3 (R represents a trivalent rare-earth ion) family, it was pointed out that the interfacial electronic properties and magnetism can be effectively tailored by the specific choose of R. 11,[16][17][18] Based on this, it can be conjectured that similar behavior can be achieved by substituting Sr with a divalent alkaline earth ion, A in RTiO 3 /ATiO 3 superlattices 19 . Up to date, however, there is no experimental information on whether any RTiO 3 /ATiO 3 interface outside of STO support metallic ground state.…”
mentioning
confidence: 99%
“…[3][4][5][6][7] Most studies thus far have focused on 2DEGs at polar/nonpolar interfaces, such as LaAlO 3 / SrTiO 3,[8][9][10] LaTiO 3 /SrTiO 3,11,12 and GdTiO 3 /SrTiO 3.…”
mentioning
confidence: 99%