Back-To-Back Changes In General Genus Of Expansion

Let us say that there was an initial substringular activity, that were to then work to cause a relatively chaotic substringular-based Rayleigh-scattering-associated implosion, that would here happen to an initially relatively organized grouping of what would here be a set of orbifold eigensets -- that were then initially harmonic in their relative delineations, as individually taken eigenindices that worked to form an initially Reimman configuration of a Majorana-Weyl-Invariant-based mode in time and space.  The ensuing so-stated Rayleigh-based implosion, that would then happen as an annharmonic scattering of an initially ordered Reimman set of orbifold eigensets -- of which, although the said annharmonic scattering were to work to pull the eigenindices of the said set of orbifold eigensets closer together, as an overall proximal localized set of Hamiltonian operators that had been put into a relative scalar magnitude of entropy, such an annharmonic scattering would tend to cause the adjacent of such so-eluded-to eigenindices to bear an odd chirality -- after the so-stated chaotic activity were to here occur.  Let us then say that there was to next off be a binary tense of a mode, as to the ensuing expansion of the Poincare-based locus of the correlative eigenmembers that had just been pulled inward in a chaotic manner -- to where this cross-product-based resulting outward thrust would be a sequence of what would first be a Clifford Expansion as to the mode of the proximal delineations of the original eigenmembers of the orbifold eigensets, of which would then move into a euclidean expansion of the so-stated original eigenmembers of the self-same orbifold eigensets, to where this works to become a back-and-forth successive series as to the mode of the expansion of what were initially the Yukawa-based existence of the eigenmembers of the said set of orbifold eigensets, by which the earlier mentioned tense of activity that had happened in so as to be caused by the chaotic implosion of the initially harmonic ordering of the eigenmembers that were of the so-stated set of orbifold eigensets, would subsequently -- via the gauge-metrical Hamiltonian operation of the said general genus -- of what would here be, in this given arbitrary case, the sequential expansion mode -- in so as to work to form what is to here become an asymptotic approach of a Reimman scattering, -- to where, although the whole initial tendency as to the gambit of each of the initially directly corresponding eigenindices of the said set of orbifold eigensets, will here not be able to, by such a said respective given arbitrary means, work to bear all of such said eigenindices to spontaneously, by this method, be able to all bear adjacent eigenmembers that would be of an even chirality -- theoretically, then, the directly correlative Njenhuis spin-orbital tensors that would here act as Li-associated oscillation-based Hamltonian operators, would here approach a closer and closer scalar amplitude as to bearing the desired perfectly even eigencondition of chirality, for all of the correlative respective eigenindices of such a case.  Yet, the covariant activity of external forces would tend to cause an impending Yukawa interaction -- that would then tend to spontaneously cause what I had just said would continue to move in the direction as to be of the given arbitrary respective case, in theory, to instead, change in its mode -- over an ensuing series of group-related instantons, -- particularly if there is a relatively transient duration into which the said set of orbifold eigensets is to be forced into a Gliosis-based contact with the Yukawa-based torsioning of external substringular forces.  I will continue with the suspense later!  To Be Continued!  Sincerely,
Samuel David Roach.