2020
DOI: 10.1016/j.jmrt.2020.02.044
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Magnetic susceptibility, EPR, NEXAFS and XPS spectra of Fe-doped CaBi2Nb2O9

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Cited by 16 publications
(5 citation statements)
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“…[55] The g ≈4.3 value is assigned to high spin Fe 3+ with rhombic zero field splitting (E/D = 1/3), [9,55] while the weak shoulder at g ≈9.6 has been previously assigned to Fe 3+ with lower rhombicity E/D ≤1/3. [55] Finally, a broad axial signal between g = 6 and g = 2 is also observed in TAP 900@Fe, previously characterized as high spin Fe III with large axial zero field splitting owing to a square pyramidal or quasi octahedral coordination environment. [9,56] Low temperature Mössbauer spectra with an external low (60 mT) and high (7 T) magnetic field were recorded to help resolve the Fe sites, with best fit simulations yielding five separate Fe assignments (Figure 5d and Table S5, Supporting Information).…”
Section: Resultsmentioning
confidence: 97%
See 1 more Smart Citation
“…[55] The g ≈4.3 value is assigned to high spin Fe 3+ with rhombic zero field splitting (E/D = 1/3), [9,55] while the weak shoulder at g ≈9.6 has been previously assigned to Fe 3+ with lower rhombicity E/D ≤1/3. [55] Finally, a broad axial signal between g = 6 and g = 2 is also observed in TAP 900@Fe, previously characterized as high spin Fe III with large axial zero field splitting owing to a square pyramidal or quasi octahedral coordination environment. [9,56] Low temperature Mössbauer spectra with an external low (60 mT) and high (7 T) magnetic field were recorded to help resolve the Fe sites, with best fit simulations yielding five separate Fe assignments (Figure 5d and Table S5, Supporting Information).…”
Section: Resultsmentioning
confidence: 97%
“…Interestingly, the signal of TAP 900@Fe closely resembles EPR results from a Fe‐doped CaBi 2 Nb 2 O 9 material. [ 55 ] The g ≈4.3 value is assigned to high spin Fe 3+ with rhombic zero field splitting ( E/D = 1/3), [ 9,55 ] while the weak shoulder at g ≈9.6 has been previously assigned to Fe 3+ with lower rhombicity E/D ≤1/3. [ 55 ] Finally, a broad axial signal between g = 6 and g = 2 is also observed in TAP 900@Fe, previously characterized as high spin Fe III with large axial zero field splitting owing to a square pyramidal or quasi octahedral coordination environment.…”
Section: Resultsmentioning
confidence: 99%
“…The observation of hydrogen in the outlet stream during the TPR measurements supports hydroxyl formation and hydrogen removal. This observation is supported further as barium cerate-based proton conductors retain hydroxyl groups at higher temperatures even at 800 °C under high steam operation conditions. , Niobium in a coexisting environment with Fe is known to assume the higher oxidation state, that stabilizes the crystal lattice. , Fe has been reported to exsolve to the Fe 0 state in reducing conditions but in the presence of B site cations with higher oxidation states, Fe has been shown to remain trivalent as confirmed by XPS and NEXAFS analysis of the Fe-doped double perovskite CaBi 2 Nb 2 O 9 . , Figure S14 indicates a lack of satellite features or shouldering around a binding energy of 715 and 718 eV which have been previously shown to account for mixed Fe 2+/3+ oxidation states in La 0.6 Sr 0.4 FeO 3−δ (LSF), and SrTi 0.7 Fe 0.3 O 3−δ (STF) electrodes . Thus, Fe 3d XPS scans for all of the samples before and after TPR measurements showed the presence of Fe 3+ with no peak or satellite features observed corresponding to Fe 2+ or Fe 0 (Figure S14).…”
Section: Resultsmentioning
confidence: 64%
“…61,62 FigureS14indicates a lack of satellite features or shouldering around a binding energy of 715 and 718 eV which have been previously shown to account for mixed Fe 2+/3+ oxidation states in La 0.6 Sr 0.4 FeO 3−δ (LSF), and SrTi 0.7 Fe 0.3 O 3−δ (STF) electrodes 63. Thus, Fe 3d XPS scans for all of the samples before and after TPR measurements showed the presence of Fe 3+ with no peak or satellite features observed corresponding to Fe 2+ or Fe 0 (FigureS14).…”
mentioning
confidence: 99%
“…[39] Nb 5þ 3d 3/2 and Nb 5þ 3d 5/2 binding energy peaks are seen at 207.4 and 210.4 eV, respectively (Figure S1b, Supporting Information). [40][41][42] The main peak of S 2p (S 2p 3/2 and S2p 1/2 ) appeared at 161.5 and 163.4 eV (Figure S1c, Supporting Information), respectively. [43]…”
Section: Characterizationmentioning
confidence: 99%