“…The two strong bands at 445 and 610 cm −1 are attributed to the O-Ti-O bending vibration and asymmetric Ti-O stretching vibration, respectively. The two weak bands at 135 and 830 cm −1 are due to the rotation of the TiO6 octahedra and symmetric Ti-O stretching vibration, respectively [1,7,9,24]. In the Raman spectra collected in the in situ high-pressure experiment (Figure 6 and Table 1), three strong bands at 235, 445, and 610 cm −1 can be observed, while the bands initially located at 135, 325, 360, and 830 cm −1 can hardly be detected due to their relatively low intensity.…”