Part Two Of Session 13 Of Course 20

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.

Part One Of Session 13 Of Course 20

Electromagnetic energy, including all light, tends to scatter at least to some extent -- if that electromagnetic energy is not propagated in a perfectly orthogonal nature upon any given surface of any phenomenon that the given electromagnetic energy is interfacing upon.  Whenever any electromagnetic energy is orthogonal in both its transference and in its propagation through and/or upon a surface or region, the given electromagnetic energy is then here to be polarized, through and/or upon the given surface or region.  When electromagnetic energy -- in the form of quantized beams or waves -- is to be made orthogonal as a field, to any plain kinetic energy that is here to exist as a field, then, the said electromagnetic energy will tend to be absorbed, -- as opposed to instead being scattered.  If the given electromagnetic energy is not completely polarized, and is thus scattered, then, the electromagnetic energy that is here to be striking a tense of plain kinetic energy, must switch in its genus of light-cone-gauge topology -- right after the so-eluded-to light acts in so as to strike the surface of the given plain energy of such a given arbitrary case.  That would then mean, that the said electromagnetic energy that is scattered here, is then here to change temporarily from initially working to bear a Yang-Mills topology, into then working to bear a Kaluza-Klein topology.  This here would then mean, that the Clifford algebra here would convert from working to primarily bear both a euclidean and a hermitian geometry, into then working to involve primarily a euler and a Dirac geometry -- for the time being.  Once the given electromagnetic energy is scattered, the Gaussian of the stringular part of the light, will then switch in light-cone-gauge orientation by 90i degrees.  The torque given in the Gaussian, causes a spring-like torsioning, that is here to automate a reversal in the changed Gaussian.  As the Gaussian is switched by the said light-cone-gauge torsioning, the scattered electromagnetic energy is then to work to pull in upon itself -- to act in so as to work to cause the scattered light to requantize with the proximal local Yang-Mills topology -- that is in the here so-eluded-to substringular region.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Adjacent Superstrings Versus Adjacent Light-Cone-Gauge Eigenstates

Immediately adjacent superstrings that are of the same universe, are 90 degrees relative to one another -- whereas, immediately adjacent first-order light-cone-gauge eigenstates that are of the same universe, are 90i degrees relative to one another.

I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.