AVS 64th International Symposium & Exhibition | |
Surface Science Division | Wednesday Sessions |
Session SS-WeM |
Session: | Deposition and Growth at Surfaces |
Presenter: | Jared Bruce, University of California Irvine |
Authors: | J.P. Bruce, University of California Irvine A.D. Babore, University of California Irvine R.P. Galhenage, University of California Irvine J.C. Hemminger, University of California Irvine |
Correspondent: | Click to Email |
Model heterogenous catalysts are traditionally studied using well-defined single crystal surfaces. However, industrial applications of these catalysts do not involve well – defined crystal surfaces but are comprised of colloids and other small crystallites. Development of a more representative model system, where nanomaterials and colloids of the active catalyst material are supported on an oxide nanoparticle, will enable rigorous investigation under relevant catalytic conditions.
TiO2 is a stable oxide material that can be used to support an active catalyst material such as platinum. Our group has shown that physical vapor deposition can be used to create TiO2 nanoparticles supported on highly oriented pyrolytic graphite (HOPG). TiO2 nanoparticles are ideal for photodeposition of platinum using low concentrations of a chloroplatinate salt in aqueous conditions to control the amount of Pt deposited on the surface. Initially, the Pt deposits as a Pt (IV) oxide material as observed by X – ray photoelectron spectroscopy (XPS) and can be reduced to Pt (II) species by continued irradiation in the absence of the chloroplatinate salt in solution. Interestingly, we have not observed a complete conversion to Pt (0) and only upon heating to 400K in vacuum do we observe the presence of the Pt (0) species. We have also used temperature programmed desorption (TPD) to characterize the change in water desorption thermodynamics when Pt has been deposited on the surface of the TiO2 nanoparticles. When Pt is present on the surface, there is a shift to lower temperatures in the monolayer and second layer desorption states. The relative shift is dependent on the total amount of Pt present on the surface of the TiO2.