Partition-Based Discrepancies And Orbifold Eigensets

Let us initially consider a mass-bearing orbifold eigenset, that is here to be traveling at a constant rate -- that is here to be translated in a constant direction.  Over the whole evenly-gauged Hamiltonian eigenmetric, in which the said orbifold eigenset is to be traveling in a so-eluded-to constant velocity -- the Lorentz-Four-Contraction of the said mass-bearing orbifold eigenset is here to be maintained, when this is here to be considered as a specific scalar amplitude of a given arbitrary contraction.  This will then work to mean, that the so-eluded-to set of discrete energy quanta that are here to operate in so as to perform one specific function, will, over the proscribed metric of duration in which it is to be going at a constant velocity -- will then work here to bear a constant scalar amplitude of its directly corresponding Polyakov Action.  This will then consequently mean, that the individually taken mass-bearing superstrings that are here to work to help at comprising the said mass-bearing orbifold eigenset, will, over the course of the said Hamiltonian eignemetric, work to bear an unchanged number of partition-based discrepancies.  (Each mass-bearing superstring of discrete energy permittivity, that is to work to comprise an orbifold eigenset that is to be moving at a constant velocity -- will consistently work to bear the same number of partition-based discrepancies.)  Furthermore, since when an orbifold eigenset is to be consistent as to be working to bear the same Lorentz-Four-Contraction over a metric of duration, is to tend to neither gain nor lose mass spontaneously -- when there are here to be no other eminently pertinent considerations, that would work to help at causing an alteration in the mass of the so-stated orbifold eigenset -- then, such a mass-bearing orbifold eigenset will, over the said evenly-gauged Hamitonian eigenmetric, -- tend to be consistent at being comprised of by a constant number of mass-bearing superstrings of discrete energy permittivity. (And as an ansantz -- such a said orbifold eigenset will here, tend to be comprised of in this case, by a consistent number of mass-bearing discrete energy quanta.)  This is what would tend to be the case, in so long as there are here to be no ulterior discrete energy quanta, that would here to be becoming eminently Yukawa to the initially mentioned mass-bearing orbifold eigenset, in a Gliosisi-based manner -- to where this would then potentially work to alter the initially implied operation of the just mentioned mass-bearing orbifold eigenset.  To Be Continued!  Sincerely, Samuel David Roach.