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(Invited) Kinetics of Photocatalytic Multielectron Transfer By Nanoparticles of Bare or Catalyst-Loaded Titania

Monday, 30 May 2016: 09:20
Aqua 314 (Hilton San Diego Bayfront)
B. Ohtani (Institute for Catalysis, Hokkaido University, Graduate School of Environmental Science, Hokkaido Univ), S. Takeuchi (Graduate School of Environmental Science, Hokkaido Univ.), M. Takase (Graduate School of Engineering, Muroran Institute of Tech, Institute for Catalysis, Hokkaido University), and M. Takashima (Institute for Catalysis, Hokkaido University, Graduate School of Engineering, Hokkaido Univ.)
For heterogeneous photocatalysis, it is well known that photocatalytic oxidation of water into oxygen (O2) is induced by particulate photocatalysts in the presence of electron acceptors.  This reaction has been presumed to proceed through a four-electron (hole) process, and therefore it is expected that reaction rate depends on light intensity and particle size of photocatalyst, which influence the number of photons absorbed by one photocatalyst particle.  However such dependences have rarely been reported and discussed so far. In this study, we report light-intensity and particle-size dependences of rate of oxygen evolution from suspensions of commercial titania samples using iodate (IO3-) and iron(III) (Fe3+) ions as an electron acceptor under intense UV-LED irradiation (365 nm; < 300 mW).

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.