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- W2005134695 abstract "Current through ${(mathrm{P}mathrm{b},mathrm{L}mathrm{a})(mathrm{Z}mathrm{r},mathrm{T}mathrm{i})mathrm{O}}_{3}$ ferroelectrics on perovskite semiconductors is found to exhibit diode characteristics of which polarity is universally determined by the carrier conduction-type semiconductors. A persisting highly reproducible resistance modulation by a dc voltage, which has a short retention, is observed and is ascribed to a band bending of the ferroelectric by the formation of charged traps. This interpretation is consistent with a large relaxation current observed at a low voltage. On the other hand, a reproducible resistance modulation by a pulse voltage, which has a long retention, is observed in metal/${(mathrm{P}mathrm{b},mathrm{L}mathrm{a})(mathrm{Z}mathrm{r},mathrm{T}mathrm{i})mathrm{O}}_{3}/{mathrm{SrTiO}}_{3}:mathrm{Nb}$ but not in metal/${(mathrm{P}mathrm{b},mathrm{L}mathrm{a})(mathrm{Z}mathrm{r},mathrm{T}mathrm{i})mathrm{O}}_{3}/{(mathrm{L}mathrm{a},mathrm{S}mathrm{r})}_{2}{mathrm{CuO}}_{4}$ and is attributed to a possible band bending due to the spontaneous polarization $(P)$ switching. The observed current voltage $(mathrm{IV})$ characteristics, the polarity dependence, the relaxation, and the modulation are explicable, if we assume a $pensuremath{-}n$ or a $pensuremath{-}p$ junction at the ferroelectric semiconductor interface (p: hole conduction type, n: electron conduction type). The analysis suggests that an intrinsically inhomogeneous P $(ensuremath{nabla}P)$ near the ferroelectric/metal interface is likely very weak or existing in a very thin layer, when a reaction of the metal with the ferroelectric is eliminated. Additionally, the various aspects of transport through ferroelectrics are explained as a transport in the carrier depleted region." @default.
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- W2005134695 title "Electrical transport through<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=normal>Pb</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant=normal>Z</mml:mi><mml:mi mathvariant=normal>r</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant=normal>T</mml:mi><mml:mi mathvariant=normal>i</mml:mi><mml:mo>)</mml:mo><mml:mi mathvariant=normal>O</mml:mi></mml:mrow><mml:mrow><mml:mn>3</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:…" @default.
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- W2005134695 doi "https://doi.org/10.1103/physrevb.59.11257" @default.
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