2012
DOI: 10.1016/j.ijhydene.2011.04.216
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Ionic conductivity, structural and thermal properties of Ca2+ doped Y2Ti2O7 pyrochlores for SOFC

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Cited by 38 publications
(8 citation statements)
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“…The Ca–O peak around 300–400 cm –1 is not observed in the band. The presence of a band around 2350 cm –1 in the YCGO sample can be attributed to the Ca–O bond . The peak around 870 cm –1 present in the YSGO sample is assigned to the Sr–O bond, and the kink around 860 cm –1 is assigned to the Ba–O bond …”
Section: Resultsmentioning
confidence: 93%
“…The Ca–O peak around 300–400 cm –1 is not observed in the band. The presence of a band around 2350 cm –1 in the YCGO sample can be attributed to the Ca–O bond . The peak around 870 cm –1 present in the YSGO sample is assigned to the Sr–O bond, and the kink around 860 cm –1 is assigned to the Ba–O bond …”
Section: Resultsmentioning
confidence: 93%
“…The conductivity plots of the sample also show prominent transition after 600 °C. These transitions can be associated with the higher oxygen vacancy content in the sample at high temperatures [34]. The conductivities obtained previously for the pyrochlore structured Er 2 Ti 2 O 7 at 1000 °C is 1.3•10 -2 S•cm -1 [35].…”
Section: Resultsmentioning
confidence: 67%
“…14 Moreover in pyrochlores, cation or anion disorder may give rise to order-disorder transitions inuencing also the conductivity and the presence of metal-insulator transitions. 7,[15][16][17] This phenomenon is coherent with the pyrochlores predisposition towards full or partial disorder, structural distortion and phase transition from pyrochlore to a defect uorite structure. 6,18 In this general framework, doping Y 2 Ru 2 O 7 with Zn 2+ results in mixed charge at both A and B cationic sites and consequently a ruthenium mixed valence 4+/5+ is present.…”
Section: Introductionmentioning
confidence: 64%
“…5,9 On the other hand, in the case of Y 2Àx Ca x Ru 2 O 7 it has been shown that the substitution of Y 3+ by the larger Ca 2+ signicantly inuences both the magnetic and the conductive properties. 15 At present, there is not an exhaustive view of the effective role of the A site doping since this depends on the chemical nature, valence and occupancy of dopants, and on their ionic radius, magnetic conguration and stereochemical impact. In a recent EXAFS experiment on the related undoped compound Y 2 Ru 2 O 7 , 6 we found evidence of: (i) a large magnetoelastic coupling pointed out by a huge and broad peak in the Debye-Waller factor s 2 for the Ru-O(1) rst coordination shell in the temperature region around the antiferromagnetic transition at T N x 77 K; (ii) an axial distortion of the RuO(1) 6 octahedra above a critical temperature T* x 150 K which was attributed to a precursor order-disorder (OD) transition.…”
Section: Introductionmentioning
confidence: 99%