Partitions And Mini-Stringular Segmentation

Let us initialy consider a bosonic suprstring of discrete energy permittivity, that is Lorentz-Four-Contracted by a factor of 10,000.  If this is the case, then, this so-stated superstring will thereby bear the scalar magnitude of the correlative Polyakov Action by a factor of 3*10^4. If a given arbitrary superstring of discrete energy permittivity bears, over the course of one iteration of BRST, the scalar magnitude of its directly corresponding Polyakov Action by a factor of 3*10^4, then, it will work to have implemented upon it, over the course of this said iteration of BRST -- 3*10^4 of what I happen to call as "partitions."  When a bosonic superstring of discrete energy permittivity bears 3*10^4 of these so-eluded-to separations from a condition of working to bear a unitized Lagrangian-based flow -- then, this tense of a Laplacian-based differentiation of such  so-eluded-to multiple  proximal localized spots that each work to bear one of such "partitions" -- that are homotopically bound to the holonomic substrate of the topological surface of the said superstring, in a Gliosis manner at the Poincare level to the external main surface of the core-field-density, that is of that so-stated respective given arbitrary superstring, -- to where the overall net effect of the total said 3*10^4 partitions, will then work to intertwine with the said main surface of the core-field-density of this string -- as a metric-gauge-based phenomenology that operates here, in so as to bring a respective net flow in this case, of 3*10^4 times as much of the scalar amplitude of a net flow of mini-stringular segmentation that is here to be directed into the Ward-Neumman bounds of the core-field-density of the said string, than the scalar amplitude of a net flow of mini-stringular segmentation that is instead to here be directed out of the Ward-Neumman bounds of the core-field-density of the said string.  Such a net of incoming mini-stringular segmentation is to here be imbued upon the so-stated bosonic superstring of this case, in the form of those first-ordered point particles that work here in so as to help to comprise the eigenindices of the said bosonic string of discrete energy permittivity.