We have successfully measured the vacuum ultraviolet (VUV) laser photoionization efficiency and pulsed field ionization-photoelectron (PFI-PE) spectra of cold titanium dioxide (TiO2) prepared by a supersonically cooled laser ablation source. The VUV-PFI-PE spectrum thus obtained exhibits long progressions of the v2+(a1) bending and the combination of v1+(a1) stretching and v2+(a1) bending vibrational modes of the TiO2+($\tilde {\rm X}{}^2{\rm B}_2$X̃2B2) ion. The pattern of Franck-Condon factors observed indicates that the O–Ti–O bond angle of the TiO2+($\tilde {\rm X}{}^2{\rm B}_2$X̃2B2) ion is significantly different from that of the TiO2($\tilde {\rm X}{}^1{\rm A}_1$X̃1A1) neutral, whereas the change of the Ti–O bond distance is very minor upon the photoionization transition. The analysis of the PFI-PE bands has made possible the determination of the adiabatic ionization energy for TiO2, IE(TiO2) = 77215.9 ± 1.2 cm−1 (9.57355 ± 0.00015 eV), the harmonic vibrational frequencies, ω1+ = 829.1 ± 2.0 cm−1 and ω2+ = 248.7 ± 0.6 cm−1, and the anharmonic coefficients, χ11+ = 5.57 ± 0.65 cm−1, χ22+ = 0.08 ± 0.06 cm−1, and χ12+ = −4.51 ± 0.30 cm−1 for the TiO2+($\tilde {\rm X}{}^2{\rm B}_2$X̃2B2) ground state.