The FTIR spectra (Fig. 1) of P25 and the modified TiO
2 samples were analyzed to examine the existence of the functional groups. For P25, the wide peak between 900–400 cm
–1 belongs to the Ti–O–Ti stretching vibration [
22]. The other wide peak at 3600–3200 cm
–1 is very weak and ascribed to the stretch of hydroxyl groups on the surface of TiO
2 (P25). The peaks for the copious groups in the functionalized TiO
2 samples appear in the FTIR spectra. The broad peak in the range of 3600–2500 cm
–1 is attributed to the vibration of –OH in carboxylic group. The peaks for –NH
2 stretching vibration (3450–3220 cm
–1) and strong peak of –OH group are overlapped in this broad range of the spectra of EDA-TiO
2 and DLA-TiO
2. A broad and strong peak at 1690 cm
–1 in the spectrum of OAD-TiO
2 is ascribed to the C=O stretching vibration of saturated dicarboxylic acid. The peaks at 1620 and 1430 cm
–1 are related to the asymmetric and symmetric bending vibrations of COO
– group, respectively. The value of
Dn (COO
–) for the OAD-TiO
2 sample is approximate 190 cm
–1, which illustrates a bridging structure between OAD and TiO
2 [
23–
25]. The peak at 1288 cm
–1 corresponds to the stretching vibration of C–O bond. While for the EDA-TiO
2 and DLA-TiO
2 samples, N–H bending vibration of primary amine are observed at around 1620 cm
–1. The peak at 1510 cm
–1 (only for EDA-TiO
2, which is not found in the spectrum of DLA-TiO
2)is ascribed to the deformation vibration of N–H in the secondary amine, which indicates there is hydrogen bonding between the amino group and TiO
2 [
19]. The bond at 1326 cm
–1 (for EDA-TiO
2) is assigned to the stretching vibration of C–N [
26]. At the spectrum of DLA-TiO
2, the peak belonging to C=O disappears, which might be caused by the binding of the carboxyl in the DLA and the TiO
2 with chelation [
23]. The analysis of FTIR results demonstrates the existence of carboxyl and amino groups and success of TiO
2 functionalization.