The La 2−x Nd x Mo 2 O 9 (x = 0.4, 0.6, 0.8, 1.0) ceramics were successfully synthesized via the sol-gel method. Structural and microstructural analyses revealed that all the samples crystallize in the cubic phase and exhibit dense microstructures, although their particle sizes vary. Dielectric, impedance, and electric modulus spectroscopic analyses revealed two relaxation processes in both the temperature and the frequency spectra. Further investigation clarified that the two relaxation processes are associated with grain and grain-boundary relaxation. At temperatures less than 683 K, the bulk response is a localized relaxation process, whereas long-range conductivity dominates when the temperature is increased to 713 K. Traditional oxide ionic conductors, typified by yttrium-stabilized zirconia (YSZ) ceramics, have been widely applied in numerous fields as solid electrolytes.1 However, the intrinsic shortcomings of traditional oxide ionic conductors, such as their high operating temperatures, tendency to exhibit electrode sinter degradation, tendency to undergo interfacial reactions, and unstable thermal expansion coefficient, 1 compel the development of new oxide ionic conductors. La 2 Mo 2 O 9 , as a novel oxide ion conductor, has been widely studied 2 since it was discovered to exhibit high oxide-ion conductivity at relatively low temperatures (600-800• C). 3,4 As a result of the potential applications of La 2 Mo 2 O 9 as components of solid oxide fuel cells, oxygen pumps, oxygen sensors, and oxygen-permeable membrane catalysts, its oxide-ion conductivity has been investigated in depth. 5,6 The ionic conductivity of cubic-phase La 2 Mo 2 O 9 can reach 0.06 S/cm at 800• C, 3,4 which is comparable with that of YSZ at 1000 • C, 7 thus rendering La 2 Mo 2 O 9 a perfect conductive material with excellent oxygen-vacancy diffusion characteristics.8 However, the first-order phase transition that occurs in pure La 2 Mo 2 O 9 at approximately 580• C from a lower-temperature monoclinic phase to a higher-temperature cubic phase 2-4 results in a one-order-of-magnitude decrease in ionic conductivity at lower temperatures. Moreover, the dramatic change in the lattice constant induced by the aforementioned phase transition decreases the mechanical stability of devices.1,8 Therefore, suppressing this phase transition and maintaining the higher-conducting phase at lower temperatures is of great practical importance. Doping has been demonstrated to be an effective strategy for this purpose. For example, La 2 Mo 2 O 9 assumes its monoclinic phase when the Nd 3+ doping percent is less than 15%, whereas it can convert into its cubic phase when the doping percent exceeds 15%. 9 In addition, the cubic-phase crystalline material might have important applications in lasers and in the fabrication of transparent ceramics.10 Such reports inspired us to explore the intrinsic defects and related properties of Nd 3+ -doped La 2 Mo 2 O 9 , although the effect of Nd doping on the ionic conductivity of La 2 Mo 2 O 9 has been revealed in prev...