Figure 1 shows the light-intensity dependence of rate of O2 evolution from a suspension of rutile (Tayca MT-150A; 13 nm) with Fe3+. A higher-order non-linear dependence was observed in the relatively lower (< 190 mW = threshold intensity, Ithr), while the rate was almost proportional to the intensity (with slope, a) in the higher intensity range, and those dependences could be reproduced by second and first-order equations, respectively. Similar bimodal dependences, with different a and Ithr, were also observed when the other titania samples were used in the presence of IO3- or Fe3+. Assuming a kinetic model (Scheme 1) in which second-photon absorption by a one photon-absorbing particle (TiO2(h+)) within its lifetime leads to oxygen evolution, a rate equation (eq. 1) was derived using parameters of lifetime of TiO2(h+), secondary photon-absorption efficiency and rate constant of oxygen evolution by a two-photon absorbing particle(TiO2*), and further derivation for lower and higher intensity limits to eqs. 2 and 3, respectively, reproduced the bimodal light-intensity dependences. Threshold intensity (Ithr) at which order of light-intensity dependence formally changes from second to first is defined as intensity for the equal rates of eq. 1 and 2 are equal. Differences in Ithr and a depending on the kind of electron acceptors, crystalline structure (anatase or rutile) and particle size are discussed.