2013
DOI: 10.1504/ijnp.2013.054992
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TiO<SUB align="right">2 thin films studied by FTIR, AFM and spectroscopic ellipsometry

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Cited by 13 publications
(6 citation statements)
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“…The OH stretching and bending vibrations of silanol groups (Si–OH) were observed by the band at 3400 cm −1 while the 1600 cm −1 band was attributed to the bend vibrations of H– O –H bonds for the water molecules on the surface of the zeolite [ 33 , 39 ]. For TiO 2 , a remarkable band was observed at 500 cm −1 corresponding to anatase titania and in agreement with the XRD of solgel TiO 2 [ 40 ]. Rahman et al [ 17 ] reported the same FTIR spectrum for TiO 2 including two close bands for 2500 cm −1 .…”
Section: Resultssupporting
confidence: 76%
“…The OH stretching and bending vibrations of silanol groups (Si–OH) were observed by the band at 3400 cm −1 while the 1600 cm −1 band was attributed to the bend vibrations of H– O –H bonds for the water molecules on the surface of the zeolite [ 33 , 39 ]. For TiO 2 , a remarkable band was observed at 500 cm −1 corresponding to anatase titania and in agreement with the XRD of solgel TiO 2 [ 40 ]. Rahman et al [ 17 ] reported the same FTIR spectrum for TiO 2 including two close bands for 2500 cm −1 .…”
Section: Resultssupporting
confidence: 76%
“…Both the air-TNT and H 2 -TNT groups showed broad bands ranging from 500 to 1000 cm −1 , which are caused by the Ti–O–Ti stretching vibration of Ti ions with octahedral coordination in anatase TiO 2 . 11 , 32 The band between 500 and 1000 cm −1 was weaker and broader in the H 2 -TNT spectrum than in the air-TNT spectrum, which might be related to nonstoichiometry caused by oxygen vacancies. 11 When compared with the air-TNT spectrum, an additional small peak at 1640 cm −1 and a broad band at 3400 cm −1 were observed for the H 2 -TNT spectrum, which might be attributable to the fundamental stretching vibration of absorbed water and/or –OH groups on the surfaces of the nanotubes.…”
Section: Resultsmentioning
confidence: 95%
“…11 When compared with the air-TNT spectrum, an additional small peak at 1640 cm −1 and a broad band at 3400 cm −1 were observed for the H 2 -TNT spectrum, which might be attributable to the fundamental stretching vibration of absorbed water and/or –OH groups on the surfaces of the nanotubes. 11 , 3234…”
Section: Resultsmentioning
confidence: 99%
“…Absorption at 385 and 438 cm –1 can be attributed to the Ti–O–Ti bonds of the anatase phase of TiO 2 , whereas absorption at 610 cm –1 can be attributed to the same for the rutile phase of TiO 2 . The feature at 890 cm –1 can be assigned to the C–C skeleton, whereas the features at 1107 and 1725 cm –1 are due to C–O stretching modes. Absorption at 1534 and 2370 cm –1 are attributed to the vibration of C–H and CH 2 bonds, respectively, and absorption at 3750 cm –1 is due to octahedral vacancies and is designated as the Ti–OH bond. It can be observed from Figure b that the absorption related to the C–H and –OH bonds is increased slightly in the case of STOPM compared to that of STO. This increase can be attributed to the incorporation of C–H and −OH functional groups into STOPM through the addition of PMMA.…”
Section: Resultsmentioning
confidence: 99%