By the way, -- the general condition of the torsion that alters the order of any one said light-cone-gauge eigenstate by 90i degrees, works to cause the correlative composite second-order light-cone-gauge eigenstates to either go from working to bear a sinusoidal delineation -- to working to bear a relatively supplemental delineation, when there is a light-cone-gauge perturbation that is to go from working to exhibit a Yang-Mills or non abelian light-cone-gauge topology, to working to exhibit a Kaluza-Klein or abelian light-cone-gauge topology, or, in the ulterior case, to cause the composite second-order light-cone-gauge eigenstates to go from working to bear a relatively supplemental delineation, to working to bear a sinusoidal delineation, when there is a light-cone-gauge perturbation that is to go from working to exhibit a Kaluza-Klein or abelian light-cone-gauge topology to a Yang-Mills or non abelian light-cone-gauge topology. Such a said torsioning is necessary, in order to work to allow for electromagnetic energy to initially to be able to re-arrange as entropic photons, when it is first disorganized by a correlative scattering -- while to then to be able to re-group and re-quantize as non entropic photons, once such electromagnetic energy has torsioned back into the general genus of the proximal local electromagnetic radiation. Once the multiplicit photonic energy is to be re-quantized back into the general proximal local electromagnetic radiation, in so as to here to be having a Yang-Mills light-cone-gauge topology -- its Clifford algebra will then have more of a tendency of going from working to bear a primarily euler and a Dirac geometry, into working, instead, to bear a primarily euclidean and a hermitian geometry, over time.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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