When The Polyakov Action Is Not Perturbative

Let us initially consider a given arbitrary orbifold eigenset, of which is here to be comprised of by the presence of mass-bearing superstrings of discrete energy permittivity.  The multiplicit Polyakov Action of these composite superstrings, is here to bear a respective tense, that is currently here (over a correlative evenly-gauged Hamiltonian eigenmetric) to not be of a perturbative nature.  During the course of such an inferred correlative sequential series of group-related instantons (which is here to be over the course of the earlier implied evenly-gauged Hamiltonian eigenmetric), the composite superstrings of discrete energy permittivity -- are here to each, when individually taken, to work to bear an iterative tense of the Polyakov Action, that is here to not be in the process of being perturbated.  Since the correlative tense of the Polyakov Action, that is here to be applied to the covariant fluctuation of the topological statum of such implied strings, is here to be maintained in its scalar amplitude, for the effectual import of the correlative conservation of homotopic residue of this particular case, when this is here to be taken in terms of the directly corresponding attribute, by which the correlative Lorentz-Four-Contraction that is here to be applied to the eminent condition of such said strings, is here to currently be maintained, to where this will consequently work to mean, that the relative motion of these said composite strings, when in their relationship to both the presence and the motion of electromagnetic energy, will consequently work to be maintained.  Furthermore -- this will consequently mean, that the directly corresponding i*PI(Del) Action will then, at this point in codifferentiable duration, act, in so as to tend to Not be eminent in its kinematic translation, over the so-eluded-to proscribed duration of time, in which the said respective tense of the Polyakov Action is here to Not be in the process of altering for these said superstrings of discrete energy permittivity, that are here to work to comprise the earlier mentioned orbifold eigenset of such a given arbitrary case.  To Be Continued!  Sincerely, Samuel David Roach.