Tuesday, March 5, 2013

A Little Bit More As to Mass Energy Equivalence

Hello, my name is Samuel Roach. First of all, when electromagnetic energy scatters upon a mass, the action here is a Calabi-Yau interaction -- whose sub-space of interaction is a Calabi-Yau Space. Yet, the mass that is struck by a given electromagnetic energy is -- within the mass' orbifold in this case -- is Yau-Exact when in terms of the  superstrings that have  light-cone-gauge eigenstates that have a Kaluza-Klein topology. Normally, electromagnetic energy has a light-cone-gauge topology that is Yang-Mills, yet, within the duration of relatively few instantons once this given arbitrary EM energy initially has struck the mentioned mass, its light-cone-gauge topology briefly converts to a Kaluza-Klein topology that consequently converts the configuration of the said light's orbifold to be temporarily virtually Yau-Exact until the described electromagnetic energy begins to requantize back into a beam of photons. Such a tranformation of the Yau-conditions of this EM energy -- as well as such a transformation of the light-cone-gauge topology of the same arbitrarily described EM energy -- happens to any photon over a brief number of instantons when such photons initially scatter upon anything. This happens over the duration of 384 group instanton that is here directly affiliated.  Yet, unscattered quantized photons are partially Yau-Exact and Yang-Mills. The factor that makes initially scattered photons very different from substringular regions that bear mass, is that the initially scattered photons are surrounded by a Yang-Mills eigenset of orbifolds that are partially Yau-Exact in a manner that allows these scattered photons to be briefly tachyonic without having all of the mass in the universe due to an "insulated border" of the described eigenset that pulls these photons back into quantized EM energy. Mass, on the other hand (yet not in a worm-hole) is always completely Yau-Exact and of a Kaluza-Klein light-cone-gauge topology. Orbifold eigensets of a mass are in a static equilibrium that forms a local conformal invariance that is covariant, codifferentiable, and codeterminable with its surroundings -- based on more of a direct wave-tug placed upon it by the Rarita Structure via the Ricci Scalar as well -- even though the here related orbifold eigensets bear an exterior that is Yang-Mills yet Yau-Exact. If I make any inadvertant mistakes, let's form a dialogue, and we will learn together.  I will continue with the suspense later!  Sincerely, Sam Roach.

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