2020
DOI: 10.1103/physrevresearch.2.042040
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Local polarization in oxygen-deficient LaMnO3 induced by charge localization in the Jahn-Teller distorted structure

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Cited by 7 publications
(4 citation statements)
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“…Fig 2). We note here that this polarization is of similar magnitude as in conventional ferroelectrics such as BaTiO 3 (22 µC/cm 2 ) 54,55 . This increased polarization is accompanied by an average increase of the Mn off-centering defects.…”
Section: Interplay Between the Polar Defect Strain And Polarizationsupporting
confidence: 71%
“…Fig 2). We note here that this polarization is of similar magnitude as in conventional ferroelectrics such as BaTiO 3 (22 µC/cm 2 ) 54,55 . This increased polarization is accompanied by an average increase of the Mn off-centering defects.…”
Section: Interplay Between the Polar Defect Strain And Polarizationsupporting
confidence: 71%
“…We note here that this polarization is of similar magnitude as in conventional ferroelectrics such as BaTiO 3 (22 μC cm −2 ). 53,54 This increased polarization is accompanied by an average increase of the Mn off-centering up to about 0.3 Å (see Fig. 11 ).…”
Section: Resultsmentioning
confidence: 90%
“…Complex transition metal perovskite oxides are a versatile class of materials with a wide spectrum of functional properties. They can be insulating, semiconducting, or metallic and show technologically relevant phenomena such as magnetism, ferroelectricity, or the more exotic high-temperature superconductivity and colossal magnetoresistance. These properties are the result of a complex interplay of charge, orbital, spin, and lattice degrees of freedom and depend strongly on strain and the defect chemistry. The structural compatibility between different perovskites allows them to be stacked on top of each other, and the advances in deposition techniques enabled the fabrication of complex multifunctional heterostructures with relative ease. These heterostructures often give rise to interesting, novel, and unexpected physical phenomena emerging at the interface where materials with different structural and electronic properties meet: quasi-two-dimensional (2D) electron gas, colossal ionic conductivity, giant thermoelectric effect, or resistance switching. ,, …”
Section: Introductionmentioning
confidence: 99%
“… 1 4 These properties are the result of a complex interplay of charge, orbital, spin, and lattice degrees of freedom 1 and depend strongly on strain and the defect chemistry. 5 7 The structural compatibility between different perovskites allows them to be stacked on top of each other, and the advances in deposition techniques enabled the fabrication of complex multifunctional heterostructures with relative ease. These heterostructures often give rise to interesting, novel, and unexpected physical phenomena emerging at the interface where materials with different structural and electronic properties meet: quasi-two-dimensional (2D) electron gas, colossal ionic conductivity, giant thermoelectric effect, or resistance switching.…”
Section: Introductionmentioning
confidence: 99%