2018
DOI: 10.1038/s41467-018-02914-9
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Discovery of a magnetic conductive interface in PbZr0.2Ti0.8O3 /SrTiO3 heterostructures

Abstract: Emergent physical properties often arise at interfaces of complex oxide heterostructures due to the interplay between various degrees of freedom, especially those with polar discontinuities. It is desirable to explore if these structures may generate pure and controllable spin currents, which are needed to attain unmatched performance and energy efficiency in the next-generation spintronic devices. Here we report the emergence of a spin-polarized two-dimensional electron gas (SP-2DEG) at the interface of two i… Show more

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Cited by 20 publications
(13 citation statements)
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“…This charge leakage is due to the proximate effect that Ti-d states in PbTiO 3 are empty while Ti-d states in BPTO nominally have 0.5e per Ti atom. Such a charge leakage can be effectively prevented by replacing PbTiO 3 with PbTi 1Àx Zr x O 3 45 , which is supported by our calculations in Supplementary Fig. 6.…”
Section: Resultssupporting
confidence: 78%
“…This charge leakage is due to the proximate effect that Ti-d states in PbTiO 3 are empty while Ti-d states in BPTO nominally have 0.5e per Ti atom. Such a charge leakage can be effectively prevented by replacing PbTiO 3 with PbTi 1Àx Zr x O 3 45 , which is supported by our calculations in Supplementary Fig. 6.…”
Section: Resultssupporting
confidence: 78%
“…In contrast, the magnetization of NS103 weakens through a negative value and then increases to zero magnetization with increasing temperature. Apparently, at low temperatures, the rise in magnetization in the M-T curve of NS103 is attributable to Nd-moments 21,32 and/or the possibility of interface magnetization due to Ti atoms in the substrate 33,34 . The negative magnetization may be attributed to the coupling between the FM of Nd and the FM- c AFM of Mn phases.…”
Section: Resultsmentioning
confidence: 99%
“…A plane wave energy cutoff of 400 eV is used following refs. , The most common Hubbard U and Hund J values applied to the Ti 3d orbitals in previous DFT + U investigations of STO , were originally proposed by Pavarini et al ( U = 5 eV, J = 0.64 eV) and Solovyev et al ( U = 3.2 eV, J = 0.9 eV). Both sets of corrections were chosen on the basis of the extent of electron localization in the Ti 3d orbitals, with the former yielding full localization.…”
Section: Computational Methodologymentioning
confidence: 99%