2018
DOI: 10.1002/aenm.201800062
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Exceptionally High Performance Anode Material Based on Lattice Structure Decorated Double Perovskite Sr2FeMo2/3Mg1/3O6−δ for Solid Oxide Fuel Cells

Abstract: A novel double perovskite Sr2FeMo2/3Mg1/3O6−δ is prepared and characterized as an anode material for solid oxide fuel cells (SOFCs). X‐ray diffraction refinement reveals that Mg and Mo cations locate separately in two different B sites (B and B′ in A2BB′O6) while Fe occupies both B and B′ sites, forming the lattice structure with the form of Sr2(Mg1/3Fe2/3)(Mo2/3Fe1/3)O6−δ. The inactive element Mg doping not only endows the material with excellent redox structural stability but also triggers the creation of an… Show more

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Cited by 68 publications
(36 citation statements)
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“…[22] Introducing divalent elements (e.g.,N i 2 + ,C u 2 + ,Z n 2 + and Mg 2 + )i nto the B'-site of SFM is effective for tuning the double perovskite structure in an air atmosphere,m ainly owing to the difference in the valence states compared with high valence Mo 6 + (see the Supporting Information, Figure S1). [19,23,24] Here, we show that the substitution of Co for Mo can also stabilize the double perovskite structure in air.B yi ncreasing Co substitution in [25] The XRD peak forS FC0.2MC0.4 at 2q of 19.68 was characteristic of the double perovskite structure (Figure 2a inset). [19,23] The ds pacing was 4.53 ,w hich was calculated by using Bragg'sl aw, nl = 2d sinq,i nw hich l = 0.15406 nm is the wavelength of Cu Ka radiation and 2q = 19.68.A sd epicted in Figure 2b,R ietveld refinement conducted on the XRD data of SFC0.2MC0.4 confirmed its tetragonal structure (I4/m space group) with lattice parameters of a = b = 5.528 and c = 7.850 ,w hich agreed with those of reported B-site ordered double perovskite oxides.…”
Section: Resultsmentioning
confidence: 65%
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“…[22] Introducing divalent elements (e.g.,N i 2 + ,C u 2 + ,Z n 2 + and Mg 2 + )i nto the B'-site of SFM is effective for tuning the double perovskite structure in an air atmosphere,m ainly owing to the difference in the valence states compared with high valence Mo 6 + (see the Supporting Information, Figure S1). [19,23,24] Here, we show that the substitution of Co for Mo can also stabilize the double perovskite structure in air.B yi ncreasing Co substitution in [25] The XRD peak forS FC0.2MC0.4 at 2q of 19.68 was characteristic of the double perovskite structure (Figure 2a inset). [19,23] The ds pacing was 4.53 ,w hich was calculated by using Bragg'sl aw, nl = 2d sinq,i nw hich l = 0.15406 nm is the wavelength of Cu Ka radiation and 2q = 19.68.A sd epicted in Figure 2b,R ietveld refinement conducted on the XRD data of SFC0.2MC0.4 confirmed its tetragonal structure (I4/m space group) with lattice parameters of a = b = 5.528 and c = 7.850 ,w hich agreed with those of reported B-site ordered double perovskite oxides.…”
Section: Resultsmentioning
confidence: 65%
“…Sr 2 FeMo 1− x Co x O 6− δ ( x =0.25, 0.30, 0.35, 0.4, and 0.6, denoted as SFMC0.25, SFMC0.3, SFMC0.35, SFMC0.4, and SFMC0.6, respectively), Sr 2 Fe 0.4 Co 0.6 MoO 6− δ (SFC0.6 m ), Sr 2 Fe 0.8 Co 0.2 Mo 0.6 Co 0.4 O 6− δ (SFC0.2MC0.4), Sr 2 FeMo 0.65 Cu 0.35 O 6− δ (SFMCu), Sr 2 FeMo 0.65 Ni 0.35 O 6− δ (SFMNi), Sr 2 FeMo 0.63 Zn 0.37 O 6− δ (SFMZn), Sr 2 FeMo 2/3 Mg 1/3 O 6− δ (SFMMg) and Sr 2 Fe 0.9 Ni 0.1 Mo 0.65 Ni 0.35 O 6− δ (SFNiMNi) were synthesized using a sol‐gel method. A similar synthesis process was reported in our previous research . The powders were obtained by calcining the precursor at 1100 °C (SFMZn, 1150 °C; SFMMg, 1200 °C) in air for 5 h.…”
Section: Methodsmentioning
confidence: 86%
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