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The vibration bands at around 2803, 1381, and 1349 cm−1 are attributed to vibrations of CH2 species.
Three peaks at 2980 2870 can1 can be attributed to vibrations in C H bonds of organic components.
Absorption in the range from 1160 to 1000 cm− 1 has been attributed to vibrations of CO group.
In the ACA-500-S@PANi spectrum, the characteristic peaks at 1576 and 1493 cm−1 are attributed to vibrations of the quinoid ring and benzene ring, respectively.
Two nearby peaks at 1,350 and 1,380 cm−1 are attributed to vibrations of bridging oxygen between the [TeO3] and [TeO4] groups.
A very intense and wide complex-shaped band in the region of 1250 980 cm−1 is a superposition of several bands attributed to vibrations of Si O Si and Si O Al fragments [39].
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The most intense absorption band in this region, located at 1062 cm−1, attributed to vibration band of C-O bond, is the only absorption band of PEG200 which is faintly visible in the FT-IR spectra of IOMNPS (Fig. 5a).
There is divergence about the region at 1316 cm 1, which can be attributed to vibration of the CH2 group of cellulose [ 35].
The peak at 1650 cm−1 is attributed to the vibrations of C=O in 5-FU (Fig. 5A).
Absorption at 1580 1680 cm−1 is attributed to deformation vibrations of adsorbed water.
A peak at 670 cm−1 is attributed to bending vibrations of aromatic hydrogen.
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