Friday, August 3, 2018

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.

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