Monday, August 7, 2017

Electromagnetic Energy As A Partially Yau-Exact Phenomenology, Part One

Orbifold eigensets that are comprised, in part, by superstrings that are of discrete electromagnetic energy permittivity, that are, when individually taken, to be continuing to move through the same medium over time, tend to behave in such a manner -- to where these may here be described of as being of such a Ward-Cauchy-based state of being partially Yau-Exact.  When a beam of electromagnetic energy is continuing to travel through the same medium over time, -- the transversal-based eigenindices of any one given arbitrary respective orbifold eigenset of electromagnetic energy, -- of which are here to tend to move in the same general direction that the correlative wave-tug of the angular momentum of the composite photons, that are here to work to comprise the said given arbitrary orbifold eigenset of such a respective case, are to be directed in  -- when this is existing in a general condition of superconformal invariance -- are here to tend to generate as much cohomology as these are to degenerate, over a set extrapolated gauged group-metric.  Yet, the homotopic torsional eigenindices, that are here to move in the same general direction as the spin-orbital momentum of the said respective given arbitrary orbifold eigenset is to be directed in, are to not to tend to be of a Yau-Exact nature.  Such said torsional eigenindices, are here to tend to either generate or to degenerate significantly more cohomology than these are here to respectively degenerate or generate -- given whether or not the directly corresponding orbifold eigenset of electromagnetic energy is to either be respectively amplified or augmented Or dampened or atenuated over time, -- as this may be extrapolated over a group-related metric, that is of a Ward-Cauchy-based Kahler condition, that is here of an Even gauge-metrical functional Hamiltonian operation over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

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