Let us initially consider an orbifold eigenset of one given arbitrary nature, that is to work to bear an ellongated pulse -- as it is to be accelerated through a Doubolt cohomology, that is to bear both a set of metrical-based Chern-Simons singularities that are to each to bear a set of complex roots, as well as to also bear a set of Lagrangian-based Chern-Simons singularities that are to each to bear a set of complex roots, -- as the so-stated Doubolt cohomology is to be able to be extrapolated as having a mappable-tracing, that is to bear a general index of Ward-Polarization, that is to be generating a respective cohomology, that is to bear a larger resultant scalar magnitude of the formation of Gliosis-Sherk-Olive ghosts than the resultant scalar magnitude of the formation of Nielson-Kollosh ghosts. So, the general condition of a net generation of cohomological residue -- that is to be formed by discrete quanta of energy that are to work together in so as to perform one common Hamiltonian operation -- will tend to form a significantly higher scalar amplitude of a Reimman scattering, that is of the norm-state-projections that such discrete energy is to strike in a Gliosis-based manner, -- than the relative quanta of the scalar amplitude of that overall Rayleigh-based scattering, that is of the Gliosis-Sherk-Olive ghosts that are to be scattered out of the condition of cohomological generation, -- that would otherwise happen if the correlative Hamiltonian-related group-related discrete energy that is to here to act as one quantum, would work to form, if it were to, instead, to act as a group-attractor of cohomological degeneration.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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