When the Fujikawa Coupling is to happen, at a relatively proximal local Ward-Cauchy-based region -- an electron is to release its excess discrete energy quantum, in the form of a photon. As an ansantz, whenever the Fujikawa is to thus happen -- the eminent photon that is thus formed, is to follow a different general Lagrangian-based path, than that given arbitrary respective electron, that is here to fall back-and-forth an energy level, in so as to release a discrete quantum of kinetic energy -- in the form of a discrete quantum of electromagnetic energy. This obvious foresight is due to the following general Ward-Cauchy-based principle: The directly corresponding electron, is here to work to tend to bear the condition of being of a d-field. The directly corresponding photon that is formed by the release of an excess discrete quantum of energy -- that is expelled by the earlier mentioned electron, is here to work to tend to bear the condition of being a p-field. The d-field of an electron -- when given its general conditions of both its angular momentum and its spin-orbital momentum, -- is to bear discrete quanta of energy that work to comprise the said electron, that have one set of potential tendencies of holomorphic drive. The p-field of a photon -- when given its general conditions of both its angular momentum and its spin-orbital momentum, -- is to bear a different set of potential tendencies of holomorphic drive, than individually taken discrete energy quanta that are of a d-field, would otherwise tend to be tugged into. Such a general difference in holomoprhic-based tendencies, is one of the general Ward-Cauchy-based conditions, that works to help at causing the eminent photon, that is thus formed by an electron, to follow a different general Lagrangian-based path -- than the directly corresponding electron that is here to fall back-and-forth an energy level to produce such a respective photon, is here to have taken.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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