As To A Gliosis-Based Abelian Strike

When there is a Gliosis-Sherk-Olive cohomological-based pattern, that is formed by the physical memory of the conformally invariant motion of a set of superstrings of discrete energy permittivity -- the so-eluded-to ghost-based pattern will be of a mappable tracing, that, if this is not perturbated by an external source, will tend to be in a positioning that is relatively stationary in its Majorana-Weyl-Invariant-based mode.  Let us now say that the so-stated Gliosis-Sherk-Olive ghost-based pattern that I have mentioned here, works to bear an external-based core-field-density, that works to bear an abelian geometry, in retrospect to its exterior Yukawa-based field.  Let us now say that there will be an incoming relatively reverse-holomorphic set of norm-state-projections, that will be heading towards the Gliosis-based field of the said respective given arbitrary Gliosis-Sherk-Olive cohomological-based pattern, that is of this given case scenario.  Let us now say that one is looking, in a Laplacian-based manner, in the holomorphic direction - from the relatively general holomorphic end of the so-eluded-to ghost-based pattern of the so-eluded-to orbifold -- that had just operated in so as to perform one specific function in the substringular, up until the said respective given arbitrary orbifold had perturbated out of the general but specific locus in which it had existed in a tense of conformal invariance -- at the initially so-stated tense of Majorana-Weyl-Invariant-Mode, that I had mentioned at the beginning of this given post. Let us now say that the whole ghost-based pattern of the said Gliosis-Sherk-Olive mappable tracing -- was to bear a "perfectly" trivially isomorphic chirality with the said incoming relatively reverse-holomorphic moving set of norm-state-projections -- to where each of the so-eluded-to ghost-based indices of the said physical memory of the orbifold is to match an antiholomorphic ghost-based index of the said relatively reverse-holomorphic moving set of norm-state-projection, as the impending collision is about to happen in a dot-product-based manner -- at the Poincaire level of the holomorphic end of the ghost-based pattern that was formed by the so-stated orbifold, that had worked to form the so-eluded-to physical memory of the Hamiltonian operator that had just been perturbated-out of the general locus of where the impending collision is about to happen.  Let us, as well, say, that the topological edges of the said reverse-holomorphic set of norm-state-projections is to bear an abelian geometry, towards the core-field-density that is just external to the Gliosis-based field, that is at the Poincaire level to the interior of what is about to be the group-metrical activity of a substringular collision of integrative ghost-based eigenindices.  Let us now say that the Hodge-Index of both of the individually taken so-eluded-to sets of integrative norm-state-projections is of the same discrete quantum.  This will then cause there to be a tendency, to where, the two integrative sets of norm-state-projections will often here completely scatter in a Rayleigh-based scattering, on account of both the conditions that this will be an annharmonic scattering, and, also because such a scattering will work to cause the adjacent eigenmembers that are displaced in a perturbative manner, to be of an odd chirality -- at the Poincaire level to the point commutators that are hewn-in by the activity of that inter-connective fabric of mini-stringular segmentation, that is involved with the homotopic interplay of the directly corresponding norm-state-projections -- that work to form the correlative and needed interconnection of substringular field-density, that works to reverse-fractal into the activity of the condition of the multiplicit existence of Cassimer Invariance.
To Be Continued!  I will continue with the suspense later!  Sincerely, Sam Roach.