2007
DOI: 10.1016/j.jeurceramsoc.2007.02.015
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Raman scattering study of the high temperature phase transitions of NaTaO3

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Cited by 24 publications
(20 citation statements)
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“…Nevertheless, no trace of emission peak was observed for surface-doped sample. It is well accepted that the 5 D 0 − 7 F 0 transition is highly directed by local symmetry of cationic sites in the orthorhombic structure of NaTaO 3 that have C 1 site symmetry for Ta ions and C s site symmetry for Na ions, 35 for which the 5 D 0 − 7 F 0 transition of Eu 3+ is allowed. Having this in mind, it is possible to specify the site-selective occupation of Eu 3+ ions as a function of Na/Ta molar ratio.…”
Section: Resultsmentioning
confidence: 99%
“…Nevertheless, no trace of emission peak was observed for surface-doped sample. It is well accepted that the 5 D 0 − 7 F 0 transition is highly directed by local symmetry of cationic sites in the orthorhombic structure of NaTaO 3 that have C 1 site symmetry for Ta ions and C s site symmetry for Na ions, 35 for which the 5 D 0 − 7 F 0 transition of Eu 3+ is allowed. Having this in mind, it is possible to specify the site-selective occupation of Eu 3+ ions as a function of Na/Ta molar ratio.…”
Section: Resultsmentioning
confidence: 99%
“…The Na cation is surrounded by 12 O anions in a dodecahedral environment, the Ta cation is octahedrally coordinated by six O ions, and the O anions are coordinated by two Ta cations and four Na cations. There is presence of structural phase transitions with temperature for NaTaO 3 , and the ideal cubic phase can be observed only at temperatures above 600°C 37–44 . On the other hand, other different crystal structures, as a result of distorting the 3D framework of the linked TaO 6 octahedra, are generally observed at room temperature.…”
Section: Introductionmentioning
confidence: 98%
“…There is presence of structural phase transitions with temperature for NaTaO 3 , and the ideal cubic phase can be observed only at temperatures above 6001C. [37][38][39][40][41][42][43][44] On the other hand, other different crystal structures, as a result of distorting the 3D framework of the linked TaO 6 octahedra, are generally observed at room temperature.…”
Section: Introductionmentioning
confidence: 99%
“…We detected the main Raman band at 620 cm –1 , corresponding to the lattice vibrations of the NaO 12 cuboctahedra in NaTaO 3 (Figure ). Upon doping NaTaO 3 with Ba 2+ , additional Raman bands were detected at ∼830 cm –1 . The 830 cm –1 Raman band originated from the breathing vibrations of BO 6 octahedra in B-site substituted perovskites, AB 1– x B′ x O 3 . , In an ideal cubic perovskite ABO 3 , the BO 6 breathing mode with A 1g symmetry does not contribute to Raman scattering due to symmetry restriction.…”
Section: Resultsmentioning
confidence: 99%