Reports: AC10 46803-AC10: Heterometallic Oxides/Organics For Investigations Of Visible-Light Photocatalysis

Paul A. Maggard, North Carolina State University

The project has focused on two main areas that center around two synthetic approaches for achieving a new molecular-level structural control over the photocatalytic properties of materials: (1) incorporation of organic ligands into heterometallic oxides to enable a finer molecular-level structural control, and (2) molten-salt flux reactions for the controlled growth of metal-oxide particle sizes from nanometers up to micrometers.  These investigated materials are those previously proposed in my research plans and contain combinations of transition metals with electron configurations that create an optimal band-energy profile for visible-light absorption and resulting photocatalytic activity.  The research has been highly interdisciplinary, and participating graduate and undergraduate students have gained valuable experiences and professional skills relevant to solid-state chemistry, photoelectrochemistry, and physical and inorganic chemistry. 

Heterometallic-Oxide/Organic Hybrid Solids: Ligand Effects on the Structures and Properties of Metal-Oxides.  Understanding how to use ligand coordination geometries and sizes to modify the internal structures of metal oxides is essential for optimizing their optical and photocatalytic properties at the molecular level.  Our hydrothermal synthetic efforts this period have greatly expanded the number of coordinating ligands that can be used to direct the growth of heterometallic-oxide/organic solids (i.e., MM'OL; M/M' = transition metals with d0 and d10 electron configurations; L = coordinating ligand) in the Cu/Re, Ag/Re, Ag/V, Ag/Nb, and Cu/Nb systems.  For example, in the MReO4-based hybrids (M = Cu, Ag), about fifteen  different ligands have been used to obtain  from isolated trimeric and tetrameric cluster units in Ag3(pdc)3(ReO4)3∙1.5H2O and Cu2(pda)3(ReO4)2∙H2O to layered structures in M(bpy)ReO4 (A = Cu, Ag), and network types of structures in Cu(bpy)2ReO4∙ ½H2O, Ag(id)2ReO4, and Ag(dpa)2ReO4, to give just a few examples.  These compounds reveal bandgap sizes that range from ~2.1-2.5eV for the CuReO4(L) systems, to ~2.6-3.9eV for the AgReO4(L) systems.  Further, we have shown these new hybrids can be structurally modified via subsequent ligand insertion/removal reactions and resulting in lower bandgap sizes of ~0.3eV.  XPS measurements have been used to reveal that these bandgap changes are primarily a result of increasing their valence band energies, and thus the hybrids can maintain suitable band energy positions for the water-splitting redox reactions.  Further, we have recently had success in extending this work to new M(I)/Nb(V) (M = Ag, Cu) hybrid solids using aqueous solutions of HF as a solvent, resulting in (so far) eight new compounds, including Cu2NbOF5(pyz)2, AgNbOF4(pyz) and MNbOF4(bpy)∙2H2O with bandgap sizes in the range of 2.2 – 3.2eV.  New investigations of their optical and photocatalytic properties have been published during this time period.

Flux Synthesis of Metal-Oxides Particles:  Effects of Particle Growth on Optical and Photocatalytic Properties.  Completed research during this period included the investigation of two copper tantalates, Cu5Ta11O30 and Cu3Ta7O19, that were synthesized by both solid state and flux synthetic methods, respectively.  A synthetic route yielding Cu3Ta7O19 in high purity was found using a CuCl flux at 800oC and its structure was characterized using powder X-ray Diffraction (XRD) data (Space group: P63/m, No. 176).  The solid-state synthesis of Cu5Ta11O30 was performed using excess Cu2O that helped to facilitate the growth of single crystals and their characterization by XRD (Space group: P-62c, No. 190).  The atomic structures of both copper tantalates consist of alternating single and double layers of TaO7 pentagonal bipyramids that are bridged by a single layer of isolated TaO6 octahedra and linearly-coordinated Cu+.  The measured optical bandgap sizes of ~2.59 and ~2.47 eV for Cu5Ta11O30 and Cu3Ta7O19 were located well within visible-light energies and were consistent with their orange-yellow colors.  Each also exhibits optical absorption coefficients at the band edge of ~700 cm-1 and ~275 cm-1, respectively, and which were significantly smaller than that for NaTaO3 of ~1450 cm-1.  Results of LMTO calculations indicate that their visible-light absorption is attributable mainly to indirect bandgap transitions between the Cu 3d10 and Ta 5d0 orbitals within the TaO7 pentagonal bipyramids.

 
Moving Mountains; Dr. Surpless
Desert Sea Fossils; Dr. Olszewski
Lighting Up Metals; Dr. Assefa
Ecological Polymers; Dr. Miller