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In the frequency domain, the nearly constant loss, is characterized by aslope 1 in log of the real part of the electrical conductivity vs log frequencyplots. It can be explained by an anomalous diffusion, defined by a random walkwith the mean square displacement proportional to the logarithm of time, ratherthan being linearly proportional to time, as in normal diffusion. The presentwork suggests a random walk algorithm that leads to anomalous, logarithmic timedependence. That has been accomplished by scaling down the subsequent randomwalk displacements by a factor, 1/t^(1/2)

Nearly constant loss - the 2nd universality of AC conductivity by scaling down subsequent random walk steps by 1/t^(1/2)