Let us here initially consider a given arbitrary orbifold eigenset, that works to consist of being comprised of by mass-bearing superstrings -- that is here as an orbifold eigenset that is being translated as a Fourier-related De Rham cohomological Hamiltonian operator, that is here to not be in a tense of conformal invariance at its Poincare-related reference-frame -- that will tend to simply generate cohomology over time. Thus -- such a given arbitrary orbifold eigenset, that works to consist of mass-bearing superstrings -- that is as an orbifold eigenset that is being translated as a Fourier-related De Rham cohomological Hamiltonian operator, that is here to not be in a tense of conformal invariance at its Poincare-related reference-frame -- will tend to reverse-fractal out to simply be generating charge over time. The more of a Hodge-Index that there will then be, as to the number of discrete quanta of energy that are then to exist in the so-stated orbifold eigenset of mass-bearing superstrings, at its kinematic-varying proximal locus, that is here to be partaking in such a said cohomological Hamiltonian operation that is of the translation of the said De Rham cohomology over time -- the higher that the energy will be, in the so-eluded-to translation of charge per time. The more energy that is here to be involved with any one respective given arbitrary charge, -- the more of a potential voltage that may be designated to the electrodynamic transference of the here so-stated orbifold eigenset, of such a respective given arbitrary case.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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