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Volumn 87, Issue 8, 2013, Pages

Hard x-ray photoemission and density functional theory study of the internal electric field in SrTiO3/LaAlO3 oxide heterostructures

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EID: 84874540609     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.87.085128     Document Type: Article
Times cited : (69)

References (47)
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    • This enables us to detect core-level shifts of the order of ∼50 meV.
    • This enables us to detect core-level shifts of the order of ∼ 50 meV.
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    • +" ions. Thus, these features in HAXPES do reflect the Ti 3d populations with some fidelity, but do not provide information on the itinerant/localized nature of the electrons in the STO states.
    • + " ions. Thus, these features in HAXPES do reflect the Ti 3 d populations with some fidelity, but do not provide information on the itinerant/localized nature of the electrons in the STO states.
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    • The expected core-level broadening due to the binding energy shifts we observe (Fig. ) is within the error bars shown in Fig. .
    • The expected core-level broadening due to the binding energy shifts we observe (Fig.) is within the error bars shown in Fig..
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    • Data from
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    • Seeing as in the 25% oxygen-deficient case the DFT data predict the system to be metallic right from the outset, the change from a minor downward shift to a clear movement to higher La 5s binding energy at n>4 in Fig. is not linked to the onset of metallicity at n=4 observed in transport experiments. The fact that the yellow shaded areas in Fig. shift to the left as n increases illustrates more La 5s levels with a higher BE than is the case for the calculation for n=1, and it is also evident that this proportion increases rapidly for n>4. We speculate that one possible cause of this could be an interaction or coupling between holes in the outermost, oxygen-deficient surface and electrons at the STO/LAO interface. This interaction could be such that beyond a certain LAO thickness (here n∼4) the energetics within the LAO nearer the STO substrate changes, resulting in the acceleration in the downward trend seen in the green points of Fig. for n>4.
    • Seeing as in the 25 % oxygen-deficient case the DFT data predict the system to be metallic right from the outset, the change from a minor downward shift to a clear movement to higher La 5 s binding energy at n > 4 in Fig. is not linked to the onset of metallicity at n = 4 observed in transport experiments. The fact that the yellow shaded areas in Fig. shift to the left as n increases illustrates more La 5 s levels with a higher BE than is the case for the calculation for n = 1, and it is also evident that this proportion increases rapidly for n > 4. We speculate that one possible cause of this could be an interaction or coupling between holes in the outermost, oxygen-deficient surface and electrons at the STO/LAO interface. This interaction could be such that beyond a certain LAO thickness (here n ∼ 4) the energetics within the LAO nearer the STO substrate changes, resulting in the acceleration in the downward trend seen in the green points of Fig. for n > 4.


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