Thursday, December 1, 2016

Rate Versus Magnitude

The rate at which any respective given arbitrary second-ordered light-cone-gauge eigenstate is to vibrate -- over the course of BRST -- has a lot more to do with the Hodge-Index as to the number of Schwinger-Indices or gravity waves, are to be produced by the topological substrate of the directly corresponding first-ordered light-cone-gauge eigenstate.  The second-ordered light-cone-gauge eigenstates, that are to be directly affiliated with the condition of a Kaluza-Klein light-cone-gauge topology -- tend to vibrate a lot quicker over the course of BRST, than the second-ordered light-cone-gauge eigenstates that are to be, instead, directly affiliated with the condition of a Yang-Mills light-cone-gauge topology.  This is why phenomenology that is correlative to the Ward-Caucy-based conditions of a Kaluza-Klein light-cone-gauge topology, will always tend to produce more Schwinger-Indices or gravity waves -- than that phenomenology that is correlative to the Ward-Caucy-based conditions of a Yang-Mills light-cone-gauge topology.  Mass that is not tachyonic, will always tend to be of a Kaluza-Klein topology, and, such so-eluded-to manifolds of mass will always work to bear more of a direct association with gravity waves -- than a phenomenology that is instead of a Yang-Mills topology.  I will continue with the suspense later! Sincerely, Samuel David Roach.

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