2015
DOI: 10.1016/j.fuel.2015.01.069
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Studies on styrene selective oxidation over iron-based catalysts: Reaction parameters effects

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Cited by 29 publications
(22 citation statements)
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“…The findings state that the main modes of the Fe-O stretching vibration of α-Fe 2 O 3 appear at E g (620 and 658 cm -1 ). These modes may be overlapped with that at 690 cm -1 from Fe 3+ in distorted tetrahedral symmetry as well as Fe 3+ /Fe 2+ in octahedral symmetry from γ-Fe 2 O 3 [25]. At a high frequency region (Figure 3c), the modes attributable to the vibrations of α-Fe 2 O 3 at 1100 and 1300 cm -1 and the γ-Fe 2 O 3 at about 1370 cm -1 are not visible due to CeO 2 covering the previously mentioned iron phases, as observed elsewhere [17].…”
Section: Resultsmentioning
confidence: 98%
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“…The findings state that the main modes of the Fe-O stretching vibration of α-Fe 2 O 3 appear at E g (620 and 658 cm -1 ). These modes may be overlapped with that at 690 cm -1 from Fe 3+ in distorted tetrahedral symmetry as well as Fe 3+ /Fe 2+ in octahedral symmetry from γ-Fe 2 O 3 [25]. At a high frequency region (Figure 3c), the modes attributable to the vibrations of α-Fe 2 O 3 at 1100 and 1300 cm -1 and the γ-Fe 2 O 3 at about 1370 cm -1 are not visible due to CeO 2 covering the previously mentioned iron phases, as observed elsewhere [17].…”
Section: Resultsmentioning
confidence: 98%
“…It is noteworthy that the characteristic modes of the iron phases are at about 1100 and 1200 cm -1 (Figure 3c), which are attributed to the α-Fe 2 O 3 (R-3c (D 6 3d ) space group and γ-Fe 2 O 3 (Fd3m (O h 7 ) space group) are not evident in CFC. Clearly, this might be due to either the substitutional doping into the CeO 2 surface lattice by Fe 3+ and Fe 2+ species or the interstitial doping into the CeO 2 surface lattice, which increases the oxygen vacancies [23][24][25].…”
Section: Resultsmentioning
confidence: 99%
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