Several theoretical models are fitted to an exact wide-frequency-range data set representing a new random-free-energy, effective-medium expression for mobile-ion response at low temperatures. A continuous-time, random-walk K1 model, indirectly involving a stretched-exponential temporal correlation function, led to the best fit, much superior to those of two dielectric-dispersion models as well. Two types of approaches are compared for analyzing 0.4Ca(NO3)(2).0.6KNO(3) (CKN) experimental data covering a very wide frequency range: a simplified conventional approach, usually involving only some or all of the real part of conductivity, denoted type 1, and an approach involving nonlinear least-squares fitting of full complex data over its entire range, denoted type 2. The type-2 analysis uses a composite fitting model involving the K1 and involves 10 free parameters needed to well represent electrode polarization, conductive-system dispersion, nearly constant loss, and limiting far-infrared vibrational effects. It confirmed that the latter were purely dielectric and led to sigma '' and epsilon '' boson peaks; included a mobile-charge explanation of the nearly constant loss region; and yielded reasonable values of the K1-model fractional exponent, beta(1), and plausible values of a completely blocking double-layer capacitance. The good type-2 fit parameter estimates were used to generate extrapolated model response over a 20-decade range at complex conductivity and complex relative permittivity levels, as well as their accurate slopes over that range. The maximum slope of the log-log sigma' curve failed to approximate well the value of 2 usually inferred from data of the present type but instead led to a novel double peak with peak slope values of about 1.6 and 1.7 before decreasing to zero at the limiting far-infrared plateau region of sigma' response. Nearly constant loss was found to be well described by the series combination of the bulk high-frequency-limiting dielectric constant of the material and a translational ionic-motion constant-phase-element expression, one whose inclusion was also needed for representing low-frequency electrode polarization effects. Further, this combination should dominate the full response at sufficiently low temperatures.