2022
DOI: 10.1016/j.ceramint.2022.04.112
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Structure and emission properties of P2O5–Na2O–Pb3O4-MO, (MO = SrO, Y2O3, MoO3, Ag2O, CdO and SnO) glass and glass ceramics

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Cited by 7 publications
(2 citation statements)
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“…In the HT case, there is a broad absorption peak around 3480 cm −1 , ascribing to the stretching vibration of OH; as well as that in the PA‐HT case. The peaks at 500–700 cm −1 are ascribed to the MO, MOM and OMO bonds 38 . In HT case, the peak at 1366 cm −1 is ascribed to the vibration of NO 3− in the lamellar spacing of HT.…”
Section: Resultsmentioning
confidence: 96%
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“…In the HT case, there is a broad absorption peak around 3480 cm −1 , ascribing to the stretching vibration of OH; as well as that in the PA‐HT case. The peaks at 500–700 cm −1 are ascribed to the MO, MOM and OMO bonds 38 . In HT case, the peak at 1366 cm −1 is ascribed to the vibration of NO 3− in the lamellar spacing of HT.…”
Section: Resultsmentioning
confidence: 96%
“…The peaks at 500-700 cm À1 are ascribed to the M O, M O M and O M O bonds. 38 In HT case, the peak at 1366 cm À1 is ascribed to the vibration of NO 3À in the lamellar spacing of HT. In PA-HT case, the characteristic peak of NO 3À disappeared and the peak at 1038 cm À1 appeared ascribing to the P O bond, which demonstrates that PA has been successfully interlaminated into HT fillers.…”
Section: Characterization Of Pa-ht Fillermentioning
confidence: 97%