Let us say that an initial beam electromagnetic energy, this is to where, let's just say that this electromagnetic energy it here to be light, has just struck upon a given arbitrary set of orbifold eigensets. As the said light is to here be absorbed to an extent, into the holonomic substrate of the said set of orbifold eigensets -- a certain amount of electromagnetic energy is to then be released by the so-eluded-to atoms, that will have here needed to release their excessive energy that these said atoms have had here, just taken into their Ward-Caucy-based bounds. This will then work to help in causing the so-eluded-to Calabi-Yau manifold -- the so-eluded-to atoms of such a case, -- to both absorb and radiate a certain scalar magnitude of electromagnetic energy, over time. As the so-eluded-to group of atoms are to here be both absorbing and releasing a certain amount of electromagnetic energy, much of the electromagnetic energy that has scattered here, is to keep scattering among some of the other groupings of atoms -- that are proximal localized to the general field at which the source of the so-stated electromagnetic energy is being propagated into. (This general proximal localized field, is the overall set of orbifold eigensets of this given arbitrary case, that are being at least partially bombarded with light.) To an extent, much of the resultant electromagnetic residue -- that is here to be scattered from within the Ward-Caucy bounds of those mass-related superstrings, that work to comprise the Calabi-Yau manifold of such a case -- is in the form of infrared energy, or, in other word, in the form of heat-based photons.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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