Here we have zoomed in on a region of the attractor map for the Gaussian function. What happens here, we did not see in the logistic or sinusoidal function. We seem to have discovered some "unbifurcations". With increasing gain we pass from a region of chaos to a region where the attractor is periodic with a large period number. As gain is further increased this high order periodicity begins collapsing, as from 128 to 64 to 32 to 16 to 8 to 4 to 2 to 1. Then this single value for the attractor expands immediately to chaos at a certain value of gain.