2020
DOI: 10.1021/acs.jpcc.0c04807
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Doping Evolution of the Local Electronic and Structural Properties of the Double Perovskite Ba2Na1–xCaxOsO6

Abstract: We present a combined experimental and computational study of the effect of charge doping in the osmium based double perovskite Ba 2 Na 1– x Ca x OsO 6 for 0 ≤ x ≤ 1 in order to provide a structural and electronic basis for understanding this complex Dirac–Mott insulator material. Specifically, we investigate the effects of the substitution of monovalent Na with divalent Ca, a … Show more

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Cited by 14 publications
(9 citation statements)
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References 63 publications
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“…The Brillouin zone was sampled with a 3×3×3 k-mesh grid for the structure optimization step. The obtained lattice parameters of austenite were a=b=c=3.646 Å, that of ferrite were a=b=c=2.839 Å, and that of Fe 3 C were a=4.491 Å, b=5.030 Å, c= 6.739 Å, which agreed well with previous theoretical and experimental results [18,19]. For the calculation of XAS spectrum, the super-cell core-hole method as implemented in VASP code was used [16].…”
Section: Methodssupporting
confidence: 86%
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“…The Brillouin zone was sampled with a 3×3×3 k-mesh grid for the structure optimization step. The obtained lattice parameters of austenite were a=b=c=3.646 Å, that of ferrite were a=b=c=2.839 Å, and that of Fe 3 C were a=4.491 Å, b=5.030 Å, c= 6.739 Å, which agreed well with previous theoretical and experimental results [18,19]. For the calculation of XAS spectrum, the super-cell core-hole method as implemented in VASP code was used [16].…”
Section: Methodssupporting
confidence: 86%
“…where E tot is the total energy of the system, E Fe , E N , E B , E Al , E Ti , and E C correspond to the total energy per atom (the energy of a single atom in the bulk structure) of Fe, N, B, Al, Ti, and C elements, respectively. The values of the formation energies of bare matrixes are well match reference data [18]. energy was scanned at a 0.2 eV step for B K-edge and N K-edge and a step of 0.1 eV was set for L 2,3-edge.…”
Section: Methodssupporting
confidence: 58%
“…• In-situ characterization of materials under catalysis conditions with low-temperature data collection (freeze-quench approach, Klingan et al, 2018;Pasquini et al, 2019, Bergmann et al, 2020Smith et al, 2017) • Operando XAS on films for water oxidation reaction (OER) under electrochemistry conditions at room temperature (Smith et al, 2017;González-Flores et al, 2018) • XAS on dilute-solution (1 mM) protein samples at cryogenic conditions (Reschke et al, 2019) • Rapid-scan EXAFS (redox transitions and catalytic processes during cyclic voltammetry) • EXAFS as a function of chemical composition and/or temperature dependent EXAFS (Kesavan et al, 2020) 3 Technical data (a) XAS experiments at cryogenic (cryostat) or operando (electrochemistry) conditions can be performed in parallel using two energy-resolving detectors. (b) Rapid data readout/transfer (e.g.…”
Section: Instrument Applicationmentioning
confidence: 99%
“…Double perovskite (A 2 B′B″O 6 ) represents a unique class of materials for electrode materials in batteries, sensors, and fuel cells. These ternary compounds exhibit a wide range of physical and chemical properties, i.e., intersite charge transfer, disproportionation, and phase transformation. When the difference of charge or ionic radii between B′ and B″ cations are greater, double perovskites have ordered structures. , A 2 B′B″O 6 with rare-earth B′ and B″ cations attracts widespread attention, due to geometric magnetic frustration and high-quality superconducting thick films . Recently, reports of double perovskites continue to exhibit significant progress in magnetic order , and photoluminescence properties. , For example, the antiferromagnetic order of Ni 2+ ion moments is determined by Ln = La, Pr, Nd, Sm, Eu, Gd, and Tb in double perovskite NaLnNiWO 6 in the range of 23–30 K .…”
Section: Introductionmentioning
confidence: 99%