As To The Integration Of Superstrings Into Orbifolds

Let us here consider a given arbitrary superstring of discrete energy permittivity, that is differentiating in a Fourier-based manner through a discrete mean Lagrangian path -- in a medium that is of a "pure" vacuum-based Hamiltonian operand.  Let us next consider in this particular case, that what is here to be the general substringular region of this scenario -- is here to be composed of a relatively large Hodge-Index of other superstrings of discrete energy permittivity, these individually-based superstrings of which, as well, are also differentiating in a Fourier-based manner through a discrete mean Lagrangian path -- in which each of such multiplicit-based superstrings of this case, is, as well, in this scenario, to be going through a medium that is of a "pure" vacuum-based Hamiltonian operand.  Let us next say that there is some tense of a group-attractor, that is proximal localized in what is here to be the general substringular region in which the many superstringular metrical-gauge based Hamiltonian operators -- are here to be moving towards each others field-density, in a greater scalar amplitude of potential collision, over a relatively transient duration of time.  Let us then say, that in this respective given arbitrary case -- once the relatively large quantum of superstrings that are here to each be initially acting as their own orbifold eigenset, are here to then be infringing upon a relatively close to Gliosis-based multiplicit proximal locus to the each others core-field-density -- the velocity that each of such superstrings had been bearing, as a scalar amplitude of their relative and respective genre of Noether-based translation, will be significantly lowered in scalar magnitude, as such superstrings are then to be pulled (actually pushed, in part, by gravitational waves from the other side) into a codifferentiable, codeterminable, and in a covariant manner, in such a manner, to where all of the here so-implied superstrings of such a case -- that were initially of the respective different independent orbifold eigensets, are now to be of the same larger overall so-eluded-to orbifold eigenset.  At this point, the overall quantum as to the composition of what is now to be one larger set of superstrings, that are to then perform one group-related function -- is to then to tend to work to bear a relatively more steady-state tense of a Majorana-Weyl-Invariant-Mode, than the initially so-stated individual superstrings of discrete energy permittivity that I had started out mentioning, were to have had at the respective start of this given arbitrary case scenario.
 I wil continue with the suspense later!  To Be Continued! Sincerely, Samuel David Roach.