The Holonomic Substrate Of The Light-Cone-Gauge

Let us consider in this case, the light-cone-gauge topology that is directly associated with a fully uncontracted mass-bearing superstring of discrete  energy permittivity.  The topology of such a given arbitrary superstring, if of a Noether-based flow, will be one in which the light-cone-gauge is of a Kaluza-Kleiln-based nature.  A fully uncontracted mass-bearing superstring, will be fully decompacitified -- to the inverse of the scalar amplitude as to to how such a string is here to be fully uncontracted, over the course of a directly correlative iteration of BRST -- when such a superstring is to behave as I have here so-eluded-to.  Since the light-cone-gauge topology of such a superstring is of a Kaluza-Klein-based nature -- the inter bound twining of the mini-stringular segmentation -- that is utilized here in so as to work to form the so-eluded-to second-ordered light-cone-gauge eigenstates -- will bear a relatively supplemental Laplacian-based delineation, during the course of the respective directly associated duration of BRST, in which such a mass-bearing superstring is to be undergoing such an iteration of a Noether-based flow, during one given arbitrary individual setting of a group-related instanton.  As the respective superstring of discrete energy permittivity is undergoing a given arbitrary metrical eigenstate of the Polyakov Action -- its directly correlative second-ordered light-cone-gauge eigenstates, that are here to be directly associated with the quantum of the respective superstring's discrete energy -- will have a certain scalar amplitude of an incoming mini-stringular segmentation, that is to here be fed into the Ward-Caucy bounds of the proximal localization where the correlative superstring is to be iterating at --  in such a manner that is needed, on account of the condition that the correlative superstring is to here be undergoing the process of bearing a "maxed-out" decompactification, that is of the so-eluded-to superstring's length and mass, that will work to then bear a core-field-density of the fields of the directly associated second-ordered light-cone-gauge eigenstates, of which  is here to then be undergoing a Clifford Expansion upon the holonomic substrate of its directly affiliated so-stated second-ordered light-cone-gauge eigenstates' topological stratum.  The process in which the Polaykov Action works to decompactify the length and the mass of a mass-bearing superstring of discrete energy permittivity, is to the inverse of what we normally think of what is considered here as to being the tense of a superstring's Lorentz-Four-Contraction.  I will continue with the suspense later!  To Be Continued!  Samuel David Roach.