The search of clean alternative energy involves catalytic reforming of high-energy-density liquid fuels and conversion of environmentally toxic byproducts to relatively benign compounds. Conductivity of the catalyst may be an added plus in order to separate out the fuel. Ceria and its derivatives, in the pure and doped form, might become useful material for such catalytic reforming and conversion processes [1,2]. BaCeO 3 , though structurally very different, can be seen as a derivative of ceria as Ba-doped ceria is chemically very similar to the BaCeO 3 . Ba-doped ceria is also expected to be a potential material for catalytic reforming and conversion. Protonic conductivity for hydrogen separation might be introduced in this material by doping [3]. Catalytic reforming and conversion efficiencies strongly depend on the chemistry and surface activity of the material. In this light nanostructured materials may be more efficient than the conventional material of similar chemistry. Recently a cost-effective and chemically easy technique has been developed to synthesize pure-and doped-ceria and its derivatives [4][5][6]. In this paper the structure, growth mechanism and the chemistry of the particles will be reported. Dilute Aqueous solution of cerium nitrate hexahydrate was reacted with a dilute solution of similar strength of hexamethylene tetramine at 80°C temperature to synthesize the pure ceria nanoparticles. In order to dope the particles with La and Gd, the aqueous solutions of the nitrate salts of the metals were mixed in the reacting solution. Similarly for the synthesis of pure-and doped-BaCeO 3 , dilute aqueous solutions of the nitrate salts of the metals were reacted with an aqueous solution of hexamethylene tetramine at 80°C. The particles have been characterized by TEM. The pure-CeO 2 particles are cuboidal in shape and 10-25 nm in size (Fig. 1). High-resolution microscopy and image simulation indicates that the particles grow by ionic attachments in aqueous medium and atomic level steps are present on the surfaces. La-doping does not change the particle morphology considerably whereas the particles are of irregular shape after Gd-doping (Fig. 2). However, dynamic equilibrium between 111 and 200 surfaces are observed under high-resolution imaging condition. It is understood that surface energies of the 111 and 200 facets determine the particle shapes. EELS studies indicate that the dopants are distributed homogeneously in the particles and Ce is predominantly in the +4 state with some +3 ions present. Ba-doped ceria or the BaCeO 3 particles are also cuboidal in shape and they are 10-25 nm in size. Zr and Co doipng results in a reduced particle size by about 5-10 nm. Zr-doping also changes the particle morphology (Fig. 3 & 4). In these particles also 111 and 200 facets can be observed. Lowtemperature synthesis of several other oxide nanoparticles (e.g. La 1-x Sr x MnO 3 ) is being carried out. Microscopic investigation of their growth mechanism is underway. It can be concluded from this study that it is p...