If such an orbifold eigenset is not of an immediately viable condition of being electromagnetic energy, and if the orbifold eigenset is here to be of a mass-bearing tense, that is here to be in the process of being translocated via a tense of Noether-related flow, -- the individually taken superstrings that are here to work to comprise the said orbifold eigenset, will tend to fidget, per each individually taken iteration of group-related instanton, in one manner or another, in a way that is either Chern-Simons in a metrical-based manner or Chern-Simons in a Lagrangian-based manner, over each succeeding iteration of discrete time. This is the tending case, no matter how hermitian the interactive overall orbifold eigenset -- that works to be comprised of by all of the so-mentioned discrete quanta of energy that are here to act as such -- is here to be. So, a Rham (De Rham) cohomology, that is of an orbifold eigenset -- that is here to be comprised of by many individually taken discrete quanta of energy -- will tend to bear composite superstrings that work to make this up, that will tend to work to bear either metrical and/or Lagrangian-related Chern-Simons Invariant singularities. Sure, for one thing, just by this, due to the condition of the eminent perturbation of the torsioning of the angular momentum of the holonomic substrate, that is of the so-mentioned mass-bearing superstrings -- such a said perturbation tends to work to change the directoral-related holomorphicity of the composite superstrings, at least by a little, per instanton, and thereby, this alone will tend to perturbate the discrete tensoric field, that is most Yukawa to that Poincare-related field that is Gliosis to the core-field-density of the cohomological activity of the general multiplicit topological stratum -- that works to comprise these given arbitrary respective superstrings, in at least one manner or another to at least some degree of scalar amplitude.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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