The starry sky model of superconductive percolation part 4: transmission of order by two kinds of nucleation nodes and critical fluctuations

Why do we need a new model and what is the problem with all previous models? All previous models have described the behavior of classical electron with resistivity along path, however we have unexpected paradoxical situation in the percolation phase transition: superconductive behavior below and above the threshold. If in the complex plane one has the Julia set and the Fisher's zeros or poles, in percolation the 'special' nodes are the singularities of kinetic coefficients in real space. We have introduced a new picture of 'propagation of order' for kinetic coefficients and a new dynamic scaling region consisting of component 1 and component, 2 parts, which are interchanged (the special nodes (poles) convert in the nucleation nodes (zeros) which become again the poles in other side of the critical point) . The critical fluctuations appear as a result of singularities disappearing