2017
DOI: 10.1039/c7nr03162a
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Oxygen defect engineering by the current effect assisted with temperature cycling in a perovskite-type La0.7Sr0.3CoO3 film

Abstract: Introducing and modulating the oxygen deficiency concentration have been received as an effective way to obtain high catalytic activity in perovskite oxides. However, it is difficult to control the oxygen vacancy in conventional oxygen defect engineering due to harsh reaction conditions at elevated temperatures and the reducing atmosphere, which make it impractical for many technological applications. Herein, we report a new approach to oxygen defect engineering based on the combination of the current effect a… Show more

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Cited by 10 publications
(6 citation statements)
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“…The photoemission and EIS measurements taken together indicate a conversion of Co 4+ to Co 3+ during contact formation for the ultrathin LSCO films grown on NSTO due to the electron transfer from the n‐type substrate, resulting in hole depletion and a higher resistivity of the LSCO films. Our observations are consistent with the ones about a combined effect of current and temperature cycling in repeated measurements of L 0.7 Sr 0.3 CoO 3 thin films, which has been shown to decrease the Co 4+ /Co 3+ ratio and was related to an increase in the resistance of LSCO films …”
Section: Resultssupporting
confidence: 92%
“…The photoemission and EIS measurements taken together indicate a conversion of Co 4+ to Co 3+ during contact formation for the ultrathin LSCO films grown on NSTO due to the electron transfer from the n‐type substrate, resulting in hole depletion and a higher resistivity of the LSCO films. Our observations are consistent with the ones about a combined effect of current and temperature cycling in repeated measurements of L 0.7 Sr 0.3 CoO 3 thin films, which has been shown to decrease the Co 4+ /Co 3+ ratio and was related to an increase in the resistance of LSCO films …”
Section: Resultssupporting
confidence: 92%
“…Controllably introduced defects alter the density of localized charges, which affect the charge mobility and the response to an incident electromagnetic field and other chemicals . Based on this principle, structural defects have been engineered to control the electronic, , optical, ionic transport, adsorption, and catalytic properties of metal oxides.…”
Section: Introductionmentioning
confidence: 99%
“…The calculation gives ∼ 3.385 × 10 6 erg/cm 3 of the K A for LSCO/LSMO/LSCO trilayer at 10 K, which is more than one order of magnitude larger than that of bare LSMO film with magnetoelastic coupling interaction (∼ 10 4 erg/cm 3 ). [16,[25][26][27] Here, the positive value of K A stands for the PMA of trilayers. Following the same procedure, the M-H curve of LSCMO/LSMO/LSCMO (x = 0.7) trilayer at 10 K is obtained as shown in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…Different from LSMO, the tensile-strained La 2/3 Sr 1/3 CoO 3 thin films easily lose oxygen to form ordering of oxygen vacancies, i.e., the brownmillerite structure of La 2/3 Sr 1/3 CoO 2.5+δ (LSCO). [25,26] The P/BM interface based heterostructures can be formed by grouping the LSCO and LSMO film together, and such symmetry mismatch at the interface may possibly tune the MA of the LSMO layer. Moreover, using Mn ions to substitute Co ions can effectively modulate the lattice structure of La 2/3 Sr 1/3 Co 1−x Mn x O 2.5+δ (LSCMO) film from brownmillerite to perovskite.…”
Section: Introductionmentioning
confidence: 99%