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Interfacial Electron Transfer Dynamics for [Ru(bpy)2((4,4鈥?PO3H2)2bpy)]2+ Sensitized TiO2 in a Dye-Sensitized Photoelectrosynthesis Ce
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文摘
Nanosecond laser flash photolysis and photocurrent measurements have been used to investigate use of [(Ru(bpy)2(4,4鈥?(PO3H2)2bpy)]2+ attached to TiO2 nanoparticle films, TiO2鈭扲uII, in a dye-sensitized photoelectrosynthesis cell (DSPEC) configuration for H2 production. In these experiments, laser flash excitation of TiO2鈭扲uII and rapid injection lead to TiO2(e鈭?/sup>)鈭扲uIII with subsequent TiO2(e鈭?/sup>)鈭扲uIII 鈫?TiO2鈭扲uII back electron transfer monitored on the nsec time scale with and without added triethanolamine (TEOA) and deprotonated ethylenediaminetetraacetic tetra-anion (EDTA4鈭?/sup>) as irreversible electron transfer donors. With added TEOA or EDTA4鈭?/sup>, a competition exists between back electron transfer and scavenger oxidation with the latter leading to H2 production in the photoelectrosynthesis cell. Reduction of TiO2(e鈭?/sup>)鈭扲uIII by both TEOA and EDTA4鈭?/sup> occurs with kD 106 M鈭? s鈭?. EDTA4鈭?/sup> is a more efficient scavenger by a factor of 3 because of a more favorable partition equilibrium between the film and the external solution. Its increased scavenger efficiency appears in incident photon-to-current conversion efficiency (IPCE) measurements, in electron collection efficiencies (畏coll), and in photocurrent measurements with H2 production. Evaluation of electron collection efficiencies by transient current measurements gave 畏coll 24% for TEOA and 70% for EDTA4鈭?/sup>. The dynamics of back electron transfer are minimized, and collection efficiencies, photocurrents, and hydrogen production are maximized by application of a positive applied bias consistent with the results of I鈭扸 measurements. A pH dependent plateau is reached at 0 V at pH = 4.5 (EDTA4鈭?/sup>) and at 鈭?.4 V at pH 6.7 (TEOA). The difference is qualitatively consistent with the influence of pH on electron population in trap states below the conduction band and the role they play in back electron transfer. The excitation dependence of IPCE measurements matches the spectrum of TiO2鈭扲uII with IPCE values 3 times higher for EDTA4鈭?/sup> than for TEOA as noted above. Absorbed photon-to-current efficiency (APCE) values are light-intensity dependent because of the effect of multiple injection events and the influence of increasing trap site electron densities on back electron transfer. The key to efficient H2 production is minimizing back electron transfer. Application of a sufficiently positive potential relative to ECB for TiO2 accelerates loss of electrons from the film in competition with back electron transfer allowing for H2 production with efficiencies approaching 14.7% under steady-state irradiation.

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