Multiple Universe-Based Orbifolds

Let us say that there were a high number of orbifolds that each were initially of several different respective individual universes -- these of which decellerated as these said multiple orbifolds approached each other's Ward-Neumman physical bounds, over a discrete sequential series of iterations of group instanton.  Here, these orbifolds will -- in this given arbitrary instance under consideration -- become of the same universe.  This is once these orbifolds settle into a metrical consideration of superconformal invariance.  That orbifold, in this given arbitrary case, that worked to bear the greatest Hodge Index basis of Hamiltonian operation -- in the process of the eluded to approach of the said given arbitrary orbifolds towards each other, after a covariant, codeterminable, codifferentiable group metric -- when in terms of the directly associated multiplicit parity and chirality associated that would here be corresponding to the overall tensoric wave-tug/wave-pull that is here related to the fractals of both the directly affiliated angular momentum and spin-orbital momentum of the said orbifolds, in the kinematic projection of the diretoral path of the Lagrangian topological sway that the said orbifolds have here been traveling through over the group metric that here involves the multiplicit approach of these said kinematic physical spaces towards each other, will then here be the orbifold that will here act as the group attractor semi-group that all of the eluded to orbifolds that will have here approached towards each other over time, that will be taken as the template as to what all of the mentioned orbifolds of this given arbitray scenario will then here synchrounize their substringular vibrations to (into the intrinsic vibration of that semi-group mentioned that will here act as the predominant substringular-based template) in so that all of these said eluded to orbifolds will then alter in so as to then be of the same universe in a consideration of a condition of superconformal invariance.   At this point, all of these orbifolds will alter from each of these initially being of different Gaussian formats, into being of the same Gaussian format.  (These will alter from being each from Njenhuis subspaces into being of a common Real Reimmanian subspace.)  I will continue with the suspense later!  Sincerely, Samuel David Roach.