Ostwald
Isolation to Determine the Reaction Order
for TiO<sub>2</sub>(e<sup>–</sup>)|S<sup>+</sup>→ TiO<sub>2</sub>|S Charge Recombination at Sensitized TiO<sub>2</sub> Interfaces
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Abstract
Kinetic isolation conditions were
identified that enabled determination
of the reaction order for interfacial charge recombination at a sensitized
mesoporous TiO<sub>2</sub> thin film. An external bias was used to
maintain a fixed and known number of oxidized sensitizers, S<sup>+</sup>, or TiO<sub>2</sub> electrons, TiO<sub>2</sub>(e<sup>–</sup>)s. Pulsed laser excitation resulted in excited state injection and
the subsequent TiO<sub>2</sub>(e<sup>–</sup>)|S<sup>+</sup> → TiO<sub>2</sub>|S reaction was quantified spectroscopically.
The data provide compelling evidence that the rate law for charge
recombination under reverse bias is <i>r</i> = <i>k</i>[S<sup>+</sup>]<sup>1</sup>[TiO<sub>2</sub>(e<sup>–</sup>)]<sup>1</sup> with <i>k</i> = 5.0 × 10<sup>–16</sup> cm<sup>3</sup> s<sup>–1</sup> (∼3 × 10<sup>5</sup> M<sup>–1</sup> s<sup>–1</sup>). Under forward bias,
the data were more complex. A recombination mechanism that incorporates
a pre-equilibrium diffusional encounter between injected electrons
and oxidized sensitizers is proposed. This and previously reported
data indicate that diffusion limits recombination when the number
of TiO<sub>2</sub>(e<sup>–</sup>)s is small and electron transfer
becomes more dominant when the number is large