Different Tenses Of Cohomological-Based Settings

Let us say that there was an initial tense of a set of superstrings of discrete energy permittivity, that existed in a Majorana-Weyl-Invariant-Mode -- in so as to form a conformally invariant matrix of relatively codifferentiable and codeterminable proximal GSO ghosts (Gliosis-Sherk-Olive ghosts), these so-eluded-to ghosts or cohomological indices -- of which would then work to form a harmonic-based scattering, or, in other words, these would then here work to form a Reimman scattering of the so-eluded-to redistributed norm-state-projections, in so as to work to form an eigenset of the correlative ghost-based indices  -- that would then be brought together by the Fourier-based kinematic activity of the translation of a relatively local eigenbase of a group-attractor matrix, over time.  Such a mappable tracing of a cohomological-based setting, will then here work to bear both: a Hodge-based index of the scalar magnitude that is relating to its relative size, a differential geometry of the Laplacian delineation of the interconnection of the eigenmembers -- that would here work together in so as to form the so-eluded to ghost-based pattern, the angling of all of the topological swaying of the so-stated eigenmembers -- that would here work to form the so-stated cohomological-based pattern, the cyclic and the imbued permutations that would here work to ebb back-and-forth into the Ward-Neumman bounds of the so-stated cohomological-based pattern, and, the interdependant kinematic interplay of the overall set of the individual eigenmembers of the so-stated cohomological-based pattern -- to where this is as taken in a retrospective manner of each eigenstate of the overall so-eluded-to ghost-based pattern towards each of the other eigenstates of the said overall so-eluded-to ghost-based pattern, that I am generically describing in this given respective arbitrary case scenario.  Depending upon how this cohomological-based mappable tracing works to demonstrate what I have just here described, its resultant interaction with other eigensets of norm-state-projections will then vary likewise.  I will continue with the suspense later!
To Be Continued!  Sincerely, Sam Roach.