DOE OSTI2016
Superionic or fast-ion conductors are multicomponent solid-state systems in which one sublattice becomes mobile and exhibits extraordinarily high ionic conductivity before the melting within the solid state. Uranium dioxide (UO{sub 2}) - the fuel material of choice in most nuclear reactors - shows superionic behavior, although the mechanism of fast ion transport of the mobile oxygen ions, and its implication, is not well-understood. UO{sub 2} belongs to the category of Type II superionics wherein the conductivity rises gradually with increasing temperature, without an attendant phase change. In a recent work, using atomistic simulations and available neutron and x-ray scattering data, we have shown that all Type II superionic conductors exhibit a well-defined onset of dynamic disorder at a characteristic temperature T{sub α} = (∼2000 K for UO{sub 2}). Unlike the familiar superionic or Bredig transition temperature T{sub α} (∼2650 K for UO{sub 2}) that is associated with a second-order thermodynamic phase transition, T{sub α} represents an order-disorder (O-D) transition that marks a structural and kinetic crossover from a crystalline state to a semi-ordered state. In the temperature range between T{sub α} and T{sub λ}, the oxygen ions in UO{sub 2} exhibit jammed dynamics even though the mobile oxygen ions favor collective hopping from one native crystalline site to another. This cooperative dynamics manifests as dynamical heterogeneity (DH) - the tendency of highly mobile oxygen ions to form dynamic clusters, and dynamical facilitation (DF) - the mode of system relaxation facilitated solely through the kinetic ions transferring their mobility to neighboring ions. The jammed dynamics portrayed by the oxygen ions is similar to that observed in supercooled liquids and glassy materials, and other disordered systems such as granular media and polymers. In the current work, we probe the ionic dynamics in UO{sub 2} for the presence of another ubiquitous signature of glassy and jammed systems, namely, the one-dimensional string-like motion of the mobile species. Unlike the uncorrelated vacancy exchanges and interstitial migration in defected crystalline states, the string motion is a collective mechanism among the mobile species wherein each member of the string induces the next member to move in a correlated, sequential fashion. Using atomistic simulations, we demonstrate that oxygen ions in UO{sub 2} are transported through a string-like mechanism in the temperature range between T{sub α} and T{sub λ}, and the probability distribution of occurrence of the strings varies exponentially with string length. The discovery of string-like motion of the oxygen ions is somewhat surprising given the crystalline underpinning of the mobile species and the dynamic tendency of the oxygen ions to hop between lattice sites. In addition to dynamical heterogeneity and dynamical facilitation, our work has added one more entry, namely the occurrence of string-like transport, to the list of phenomenological similarities between superionic conductors and jammed systems. Using atomistic simulations, we have established the occurrence of string-like ionic motion among the oxygen ions in UO{sub 2} between temperatures T{sub α} - the order-disorder (O-D) transition temperature, and T{sub λ} - the Bredig transition temperature. As observed in other jammed systems, the length of the strings is observed to have an exponential distribution implying that the probability of occurrence of a smaller string is much higher than that of a longer string. Interestingly, using Temperature-Accelerated Dynamics (TAD) we have also established that string-like hopping takes place at temperatures lower than T{sub α}; these results will be published elsewhere. (authors)
11 NUCLEAR FUEL CYCLE AND FUEL MATERIALS↗