When taken along the topological surface of any given arbitrary second ordered light-cone-gauge eigenstate, that is of a non abelien light-cone-gauge topology -- the directly corresponding holonomic substrate of the Laplacian-based condition of the so-stated topological surface, that is pertinent in this respective case, is of a sinusoidal nature and Not of a supplemental-based nature, during the correlative individually taken durations of BRST that are to here be directly related to the so-eluded-to iterations of group-related instanton, by which any respective given arbitrary Yang-Mills or non abelien light-cone-gauge topology is to be interactive, when upon its Gliosis-based environment in the substringular. This is to where, to an extent, one may say that the tendency of any respective given arbitrary non abelien or Yang-Mills light-cone-gauge topology, is to be of more of a smooth-curved nature than that of an otherwise jointal-based nature -- over the course of each individually taken iteration of BRST, that is to here be directly related to each of the correlative individually taken iterations of the directly pertinent sequential series of group-related instanton. This will here work to indicate that the Laplacian-based nature of a Yang-Mills or a non abelien light-cone-gauge topology, will tend to have a relatively higher scalar amplitude of working to bear a relatively stronger elastic modulae over time -- than that of a directly comparitive Kaluza-Klein or an abelien light-cone-gauge topology -- while the Laplacian-based nature of a Kaluza-Klein or an abelian light-cone-gauge topology, will tend to have a relatively higher scalar amplitude of working to bear a relatively stronger fractal modulae over time, than that of a directly comparitive Yang-Mills or a non abelien light-cone-gauge topology.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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