Thursday, February 15, 2018

The Next Part Of Session 10 Of Course 20 -- Calabi-Based Interactions And Calabi-Based Manifolds

One can not have a fraction of an electromagnetic beam, yet, one may have a quantum of many electromagnetic beams that are quantized together.  One may have a quantum of electromagnetic energy that contains multiple types of electromagnetic energy that are integrated as one unit, which is usually the case from within the confines of a planet.  Let us say that a bunch of beams of electromagnetic energy are quantized, and are heading for an object of mass -- that is in its direct path.  The electromagnetic energy scatters, when it interfaces with the object of mass.  When the quantized beams of electromagnetic energy are about to strike the given object, the beams of energy that are here given, are to be situated with what may be termed of here as being of a Yang-Mills topology.  A Yang-Mills topology eludes to the condition -- that the Gaussian of the given light-cone-gauge is 90i degrees  to the Gaussian of the light-cone-gauge of the object of mass, that the beams of energy given are about to strike.  When the beams of quantized electromagnetic energy scatter upon the given mass, the scattered energy temporarily becomes of a Kaluza-Klein topology -- in that the Gaussian of the beams of quantized electromagnetic energy are then to be interfacing with an orthogonal Gaussian light-cone-gauge eigenstate -- that works to relate a supplemental Njenhuis set of Ricci tensors, that set a directly corresponding Klein Bottle eigenstate to interact with the Regge Slope, in so as to work to help at allowing for the correlative related phenomenology -- that is here to be going through a directly corresponding Gaussian Transformation -- to be Gliosis to the Kahler-Metric, over a relatively brief sequential series of group-related instantons.  This is here to be involved most specifically, in this given case, at the interface of the Gliosis-based interaction, that is here to exist between the said electromagnetic energy and the substances that it is to be scattering upon.  Remember, Lorentz-Four-Contractions only apply for phenomenology that have not been topologically frayed by a black-hole.  So, whenever light, or, for that "matter," whenever electromagnetic energy is to scatter, individual discrete electromagnetic quanta of energy are very transiently sped up for 384 consecutive iterations of group-related instanton, per each individually taken entropic photon that has here just respectively been scattered, while then slowed down (although such discrete electromagnetic quanta are slowed down as is according to Snell's Law, when detected by any overt means of physical extrapolation).  Such a very brief "tachyonic" propulsion, is here to be explained by the following:  Imagine a bright and hot electrostatic "ball," that is to go from traveling through a vacuum -- into traveling through a thicker medium -- all of the sudden.  As this "ball" of charge is to be going through the said thicker medium, the overall motion of the said electrostatic ball will be slowed.  Yet, the static electromagnetic energy that is at the perithery of the ball, may be imagined to very temporarily speed-up upon direct contact with the said thicker medium, while then such an external static charge will ensue, in so as to be brought back to the relative core of the said overall slowed hot electrostatic ball -- that has here to have lost velocity by moving into a relatively thicker medium.  As the photons that were very briefly made entropic, are to ensue in so as to be re-quantized with that respective beam of light -- that these had temporarily been scattered out of -- the so-eluded-to electromagnetic energy that is not "entropic," is then said to be back to having a Yang-Mills light-cone-gauge topology.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

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