The Ru(II) compounds Ru(bpy)(2)(ina)(2)(PF6)(2), Ru(deeb)(2)(py)(2)(PF6)(2), Ru(deeb)(bpy)(2)(PF6)(2), and Ru(dcb)(bpy)(2)(PF6)(2), where py is pyridine, bpy is 2,2'-bipyridine, ina is isonicotinic acid, deeb is 4,4'-(CO2Et)2,2'-bipyridine, and dcb is 4,4'-(CO2H)(2)-2,2'-bipyridine, have been prepared, characterized, and anchored to colloidal ZrO2 and TiO2 thin films for excited state and interfacial electron-transfer studies. In neat acetonitrile at 22 +/- 2 degrees C, Ru(bpy)(2)(ina)(2)(PF6)(2) is photochemically unstable and nonemissive with a short excited-state lifetime, tau < 10 ns. When anchored to ZrO2, the lifetime of Ru(bpy)(2)(ina)(2)(PF6)(2) increases to 60 ns at 22 +/- 2 degrees C and is highly temperature dependent due to the population of a low-lying state(s) that are proposed to be ligand field (LF) state(s). The LF state(s) can be populated directly from hot vibrational excited states and from the thermally equilibrated metal-to-ligand charge-transfer excited state. On TiO2 the excited-state behavior of Ru(bpy)(2)(ina)(2)(PF6)(2) is very similar to that on ZrO2, except that fast interfacial electron injection occurs, k(inj) > 10(8) s(-1) Ru(bpy)(2)(ina)(2)/TiO2 displays temperature-dependent electron injection, intersystem crossing,and emission quantum yields. A model is proposed where the direct population of LF states competes kinetically with electron injection. This behavior is contrasted with other sensitizers that have excited states localized on a surface-bound ligand.