Oxygen vacancies induce changes in lattice parameter, photoluminescence characteristics and Raman spectra of sol–gel derived fluorite-type cubic CeO2 and Ce0.8Zr0.2−xAxO2 (A = Co/Fe, x = 0–0.2) powders

An attempt has been made here to synthesized ceria (CeO 2 ) and Ce 0.80 Zr 0.20− x A x O 2 (A = Fe, Co; x  = 0–0.20) powders via novel sol–gel technique using metal nitrate hydrates as precursors and distilled water and ethanol as solvents. The resulting gel was dried at 130 °C for 24 h and calcined...

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Veröffentlicht in:Applied physics. A, Materials science & processing Materials science & processing, 2022-08, Vol.128 (8), Article 712
Hauptverfasser: Samdarshi, Shashi Kumar, Agrawal, Atul Kumar, Chauhan, Santosh, Singh, Rakesh Kumar, Kar, Manoranjan, Kumar, Jitendra, Jaiswal, Shivendra Kumar
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Sprache:eng
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Zusammenfassung:An attempt has been made here to synthesized ceria (CeO 2 ) and Ce 0.80 Zr 0.20− x A x O 2 (A = Fe, Co; x  = 0–0.20) powders via novel sol–gel technique using metal nitrate hydrates as precursors and distilled water and ethanol as solvents. The resulting gel was dried at 130 °C for 24 h and calcined successively at 850 and 950 °C for 3 h each. Ceria is shown to exhibit a fluorite-type cubic structure with a slightly higher lattice parameter a  = 5.428 Å, Z  = 4, space group Fm 3 ¯ m , some Ce 3+ ions and oxygen vacancies. 20% zirconium substitution of cerium causes decrease of ‘ a ’ to 5.395 Å owing to a lower ionic radius of Zr 4+ vis-à-vis Ce 4+ . However, the lattice parameter first increases and then decreases with partial/ full replacement of Zr 4+ by cobalt or iron ions. Evidence is found for existence disorder/strain, mismatch of ionic radii and oxidation states of cations, and appropriate oxygen vacancies to ensure charge neutrality of systems. The photoluminescence (PL) spectra reveal peaks at ~ 371, 402, and 432–445 nm, which are attributed to Ce 4f 0  → 4f 1 direct transition, Ce 4f 0  → 4f 1 electron transfer via oxygen F ++ state, and oxygen vacancies (excited oxygen F +*  → F + transition), respectively. Their Raman spectra display a peak at ~ 462 cm −1 due to F 2g symmetric vibrations of a cubic CeO 8 sub-cell with some variation in position and sharpness with/without a signal in the range 150–170 cm −1 by introduction of different cations leading to distortion and formation of anion vacancies.
ISSN:0947-8396
1432-0630
DOI:10.1007/s00339-022-05860-y