The physical topological condition of the type of wave-tug that is mapped in a Laplacian manner so as to determine the general type of differential geometry of an arbitrary given first-ordered-light-cone-gauge, that is in the state that the said arbitrary first-ordered-light-cone-gauge is in, during the sub-metric that exists here, is during the initial frame of BRST. So, if the light-cone-gauge topology that directly corresponds to a superstring bears a Kaluza-Klein topology, then, during the initial frame of sub-metric that is used to physically denote the Laplacian conditon of the start of BRST, for the here given individual superstring that is mentioned in this basic scenario, bears segments of mini-string that binds the corresponding superstring with its corelative Fadeev-Popov-Trace so as to form a field-pattern that is initially reltaively taught and non-sinusoidal -- with just enough of a leeway of "slack" so that the initial motion of the Imaginary Exchange of Real Residue fully tightens the fractal modulae of the mentioned and described mini-string that is here to be described as bearing an abelian differential geometry of substringular field. This field partial I am describing is the substrate that gauge-bosons act upon so as to form the Schwinger Indices that allow for needed covariant interactions between norm-state projections and other unmentioned superstringular phenomena. I have a lot more ellaboration where this came from!
Sorry, but I need to run now! Sincerely, Sam Roach.
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