At the Poincare level to the topological stratum, of any one given arbitrary second-order light-cone-gauge eigenstate --- right where a given arbitrary gauge-boson is acting, in so as to work to "pluck" the said second-order eigenstate -- there is a third-order Schwinger-Index, that is here to be formed during BRST. Yet, from anywhere that is outside of the region of the core-field-density -- of that discrete quantum of energy of such a case that is here to be considered, there is only the viable Ward-Cauchy-related condition of there being the existence of both first-ordered Schwinger-Indices and/or second-ordered Schwinger-Indices. (Depending upon both the manner and the scalar amplitude of the quantization of the correlative Schwinger-Indices.) The reason to this, is because -- once one is to extrapolate the general Ward-Cauchy-related condition of any viable quantization of those discrete bundles of wave, that are here o ensue, in so as to converge to be able to work to form gravity waves outside of the proximal locus where the initial Schwinger-Indices are to be formed, from their specific locus of origin -- the earlier stated third-order Schwinger-Indices will tend to always be quantized into either a second-order or a first-order Schwinger-Index.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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