Perturbative Cohomological Eigenstates

Besides the more obvious general reason as to why an initially Rham-based cohological eigenstate, is to be perturbated into the ensuing general tense of a cohomological stratum, that is known of as a Doubolt cohomology, -- as to when a Rham cohomology is to scatter upon another cohomology, in such a manner that the initially mentioned Rham cohomology is to then to tend to become, instead, of the said Doubolt-related nature, -- there is as well to be one other epifany-related additional general alterior reason -- as to why an initial Rham cohomology is to eventually become of a Doubolt nature, to where this is because of the eventual spontaneous proximal local presence of certain entities, which may be as both group-attractors and/or the proximal local presence of certain entities, which may be as ghost-inhibitors, -- to where both of such just mentioned general categories of what would generally be as the nature of being Cevita-related Hamiltonian operators, are here to have an eminent tendency of, via the innate Hamiltonian operation of the activity of their respective Fourier Transforms, to helping at causing a peturbative effect upon both the pulsation and/or the path-based flow of the so inferred orbifold eigenset, that  was to initially be functioning as a Hamiltonian operator that was here to be undergoing a Fourier Transform -- via the mappable-tracing of the initially mentioned Rham cohomology, that is here to be extrapolated as to then of becoming of a Doubolt cohomology, over an evenly gauged  Hamiltonian operation.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.