When an orbifold eigenset, that is here of one general given arbitrary case scenario, is to alter into working to bear a tense of metric-related Chern-Simons singularity -- due to the directly corresponding Lagrangian-based path of the said orbifold eigenset, to have then to be altered here, from initially working to bear a unitary Lagrangian-based path, into subsequently to be working to bear a binary Lagrangian-based path, -- this will then work at altering the directly corresponding dimensional-related pulsation of that self-same orbifold eigenset, -- over the course of that duration, in which such a said metric-related Chern-Simons singularity is to become effectual, which may be extrapolated in a Fourier-related manner, over a correlative evenly-gauged Hamiltonian eigenmetric. Consequently, whenever there is here to be a change in those correlative Yukawa-based influences, that are here to be of either a ghost-inhibitor-based nature, or of a group-attractor-based nature and/or a gauge-attractor-based nature, in which such a so-eluded-to change is then to act, in so as to influence a substantiative change or perturbation of the dimensional-related pulsation, that is here to be of the Hamiltonian-related "momentum" of the said orbifold eigenset, then, this will generally tend to work to cause the eminent proximal local presence of a set of one or more metric-related Chern-Simons singularities, along the then adjusted path-based tracing, in which the said orbifold is to then to be drawn into, due to the presence of the physical application of the earlier mentioned force-related attributes, that are here to have worked to cause such a so-inferred Yukawa-based perturbation, over the course of some respective correlative duration.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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