Tuesday, October 23, 2018

Gauge-Bosons As Messenger Particles

Gauge-Bosons work to act as messenger particles.  These said gauge-bosons act, in so as to work to pluck their correlative second-order light-cone-gauge eigenstates like a harp -- in so as to work to form a certain general genus of Schwinger-Indices, -- that are kinematic along the Rarita Structure, in so as to work to form the four general classifications of the physical forces.  Gauge-Bosons thus work to form certain given arbitrary vibrational oscillations -- that act upon their Ward-Cauchy-related substringular environment, -- in so as to help at forming these so-stated four basic physical forces of nature.  Consequently:  Where the multiplicit centralized knotting of the Rarita Structure is at, in a covariant kinematic-related manner -- due in part to the various kinematic activity of those wave-based vibrational oscillations, that are here to physically be those Schwinger-Indices that are formed by the said plucking activity of gauge-bosons -- is the multiplicit region, at which the strong force is to tend to be localized at.  Where such a said general genus of Schwinger-Indices, are to be directly associated in part with the activity of both spontaneous cohomology-based generation and/or spontaneous cohomology-based degeneration -- is where there are the multi-various eigenstates of the electromotive force to tend to be localized at.  Where such a said general genus of Schwinger-Indices are to come together, in a relatively quantized manner over time -- is where the gravitational force is here to tend to be localized at.  And, where such a said general genus of Schwinger-Indices, are to bear a general multiplicit perturbation in their covariant kinematic-based proximal locus, that is affiliated the directly correlative centralized knotting of the Rarita Structure, -- is where the weak force is to tend to be localized at.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

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