The Last Part of the Addendum Before Course 17

As I was saying in the previous post, over the course of the ensuing iterations of group instanton, that are affiliated with the sequential-based series of the recycling of norm-conditions -- via the indistinguishably different recycling of mini-string segments, that are here replaced in the so-stated indistinguishably different manner in so that there may be both an optimum fractal module and an optimum elastic modulae to be applied to the homotopic-based topological conditions of the field-density-based eigenstates that work to constitute the basis of both the inter-binding and the exterial-biding that works to comprise substringular phenomena, -- the specific indices that work to integrate in so as to form the general topology of substringular phenomena are inter-changed, in order to maintain the general condition of Cassimer Invariance.  This is part of the process that also works to inter-change the Gliossi-based conditions of smooth-curvedness with the Gliossi-based conditions of jointal-based delineation, in so that the multiplicit structural strength of the mini-string segments that work to form the basis of topology may be of an optimum quality, per regional locus, per gauge-metric, over time.  Meanwhile, with the specific case of both the previously mentioned given arbitrary one-dimensional superstring of discrete energy permittivity and the previously mentioned given arbitrary directly associated Fadeev-Popov-Trace eigenstate, the relatively linear core-field-density that was stated as being in-between the so-eluded-to discrete unit of energy permittivity and the its directly corresponding counterpart will, once that the instanton-quaternionic-field-impulse-range has begun, "evaporate" its homotopic function, until the field delineation, that the next locally derived iteration of group instanton singularizes at, at the relative field delineation that the originally mentioned "leg" of the space-hole of this given arbitrary case is -- in one manner or another -- encoded for, by the physical determination of the coefficients that work to translate such a respective genus of an eigenstate of the "space-hole," in such a manner in so that the so-eluded-to one-dimensional superstring, and, all of the other superstrings of discrete energy pemittivity of the same respective layer of reality, may keep being able to re-singularize as globally distinguishable superstrings -- that kinematically differentiate via the sequential series of their iterations and reiterations of group instanton, in such a manner in so that the said instantons, as taken individually, are like "snapshots" that are the so-eluded-to phenomena as taken in a lowered flux translation, when this is compared to the perturbative motion of what happens during the so-eluded-to directly previous field-impulse-mode -- the latter of which is the kinematic format of activity that happens 1Ihbar just before group instanton.  When such a general format of activity is going in a state of superconformal invariance, the directly related given locant neighborhood in the substringular works to form correlative eigenstates of the space-hole -- at their respective generally unnoticed gauge-metrics, that operate in so as to "vibrate" their path potential in a tightly knit region per so-eluded-to imaginary-based homotopic exchange.  This is most succinctly the case for unfrayed substringular phenomena.  To Be Continued.  Next.  Course 17.  Sam.