The following is the general tendency as to the relative Gliosis-based positioning, of those zero-norm-state-projections, that are to here act upon a quantum of discrete energy that is released as the excess energy of an electron -- in so as to result in working to form a photon (and its counterpart). In one given arbitrary case scenario, as the two individually taken sets of zero-norm-state-projections, that work to form both the respective photon and the respective counterpart of the photon -- via the Fujikawa Coupling -- are acting in a Gliosis-based manner upon the holonomic substrate of both the respective given arbitrary discrete quantum of particle-based kinetic energy permittivity, and, the respective given arbitrary discrete quantum of wave-based kinetic energy permittivity -- the so-eluded-to two open loop amplitudes, that are here of the holonomic substrate of both the respective one-dimensional superstring of discrete kinetic energy permittivity, and, the respective one-dimensional counterstring of discrete kinetic energy permittivity, are here to be closed, via the duration of a successive series of group-related instantons, in a hermitian manner -- in so as to work to help in the forming of the resultant respective said photon and the resultant respective counterpart of the so-stated individually taken photon. This said Fourier-based tense of differentiation, is to here work to form both a resultant bosonic superstring of discrete electromagnetic energy permittivity, that is completed in its formation -- at having the superstring that is to here be formed as such, to be knotted at a spot, that is here be be Gliosis to the said formed bosonic superstring, at a general locus that is proximal localized at the relative central index of curvature that is Njenhuis to the forward-holomorphic positioning of both that respective so-stated resulting two-dimensional superstring, and, at that respective so-stated resulting two-dimensional counterstring that will have here just been formed by the so-stated Fujikawa Coupling via the Green Function. This would then mean that, over the course of the Fourier-based activity of the said eigenmetric of the Fujikawa Coupling -- that the hermitian-based closing of the two said loop amplitudes, that will here result in the formation of both the here formed photon and its counterpart, will happen as a radial-based delineation of the initially so-eluded-to open-loop amplitude, in a directoral-based curvature that is here to work to bear a wave-tug based motion, that is to here be flush in the said relative Njenhuis to forward-holomorphic direction, in both of these so-stated cases. This is in so long as there is to here be no contorsioning, in what is to here be the directoral-based Lagrangian affliliated propagation of the initially so-eluded-to holomorphic direction, that is of the motion of the here formed photon and its counterpart, over the course of the said eigenmetric of the Fujikawa Coupling.
I will continue with the supsense later! To Be Continued! Sincerely, Samuel David Roach.
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