A complete critical evaluation and re-optimization of phase diagrams and thermodynamic properties of the Al 2 O 3-Ti 2 O 3-TiO 2 system at 1 atm pressure has been performed. Equilibration and quenching experiment in the Al 2 O 3-TiO 2 system in air was also performed to constrain the solubility limit of Al 2 O 3 in TiO 2 rutile solution at high temperatures. The molten oxide phase was described by the Modified Quasichemical Model considering the short-range ordering in molten oxide. While Al 2 TiO 5 and Ti 3 O 5 were treated as separate stoichiometric phases in the previous optimization, they were described in this study, using the Compound Energy Formalism, as part of pseudobrookite solid solution with a miscibility gap based on new experimental data. Corundum and rutile solutions were also described based on their crystal structures. New high temperature phase, Al 6 Ti 2 O 13 , was also considered for the first time. A set of optimized model parameters of all phases was obtained, which reproduces all available and reliable literature data within experimental error limits from 25°C to above the liquidus temperatures under oxygen partial pressures from metallic saturation to 1 atm. The newly optimized database was applied to calculate the inclusion diagram and reoxidation of Al-killed and Ti bearing steels. KEY WORDS: Al 2 O 3-TiO 2-Ti 2 O 3 ; inclusion; pseudobrookite; phase diagram; thermodynamic modeling. * Notations A, G, T are used for Al 3 + , Ti 3 + , and Ti 4 + , respectively. a The Gibbs energies pure liquid AlO1.5 (= 0.5 Al2O3), TiO2 and TiO1.5 (= 0.5 Ti2O3) were taken from and Eriksson and Pelton. 4,5) b The Gibbs energy of pseudobrookite end-members in the Ti-O system were taken from Panda and Jung. 6) c The Gibbs energy of ilmenite end-members in the Ti-O system were taken from Panda et al. 7) β,δ,φ The Gibbs energies of pure solid AlO1.5 (= 0.5 Al2O3), TiO2 and TiO1.5 (= 0.5 Ti2O3) were taken from Eriksson and Pelton. 4,5) ψ The Gibbs energies of pure rutile TiO1.5 (= 0.5 Ti2O3) were taken from Kang et al. 8)