About Perturbation of Divergent Motions

Let us initially consider two different relatively adjacent orbifold eigensets that are initially divergent -- on account of the condition that these have both just undergone a covariant Hamiltonian operation, that had worked to cause the formation of a binary Lagrangian Chern-Simons singularity upon the immediate surroundings of the field-density of each of the said individually taken orbifold eigensets, over a relatively transient duration of time. In this given arbitrary respective case, this will then cause there to be the formation of at least one metrical Chern-Simons singularity to be formed at the cite of both of such orbifold eigenstates.  Let us consider that it was the interaction of one given arbitrary ghost-based inhibitor, that had acted upon the general covariant field that had worked to inter-bind the two so-stated given arbitrary orbifold eigensets of such a case -- that had here worked to cause the said initial tense of divergence that had happened upon the Yukawa field that had worked to involve the interdependent interaction of the two said respective orbifold eigensets, during that group-metric by which the two so-stated orbifold eigensets had existed in a covariant, codifferentiable, and in a codeterminable manner, over the correlative sequential series of group-related instantons -- by which the comparison may have been able to be extrapolated.  Let us next consider -- that, after an ensuing sequence of Fourier-based differentiability had worked to interplay amongst the two said orbifold eigensets, to where this is after a brief span as to after the two so-eluded-to divergent Hamiltonian operators have become mildly more separated -- in terms of the index of the scalar amplitude of their proximal localizations in correlation with one another, there is a group-attractor that were to have here acted upon the holonomic substrate of both of the so-eluded-to Hamiltonian operators, to where one is to have a set of norm-state-projections that act in a Yukawa-based manner upon the Gliosisi-based topological stratum of the two so-stated orbifold eigensets at the Poincare level -- over a sequential series of group-related instantons, by which such a so-eluded-to Fourier-based interaction will have here worked to cause the two said orbifold eigensets that had been initially of a divergent nature, to then be pulled into a genus of what is to here form a set of reversed binary Lagrangian-based Chern-Simons singularities -- to where the two initially stated orbifold eigensets are then pulled into what is instead, of a convergent sequential series of gauge-metrical Hamiltonian operation,  this of which will then tend to work at causing the two initially said orbifold eigensets to be brought back into a closer proximal localization.  This would then work to form, as well in this given arbitrary case, a reversed set of metrical-based Chern-Simons singularities.  As the two so-stated orbifold eigensets move, in so as to converge towards one another -- there will then be a tendency of there being an increased Hodge-Index of interdependent covariant field indices, that will then work to inter-bind the general cite of there convergence, If there is a relative lack of a Yukawa-based state of a perturbative quantum entanglement that is over the course of the directly corresponding sequential series of the correlative iterations of BRST, --  in which the activity of such a metrical-based convergence is to happen in a time-wise manner.  I will continue with the suspense later!  To Be Continued!
Samuel David Roach.