Supplemental Ward-Polarization

Let us first consider here, two different second-order light-cone-gauge eigenstates -- at which each of such said second-order light-cone-gauge eigenstates are, when individually taken, struck by a gauge-boson eigenstate, in so as to work to form a third-order Schwinger-Index -- over a discrete covariant iteration of BRST.  This would then mean, that there are here, in this specific Laplacian-based localized case of both codetermination and codifferentiation, two different distinct third-order Schwinger-Indices that are being taken into consideration here, in total, in this relative respective given arbitrary case -- that are formed by by the plucking, like a harp, of two different distinct second-order light-cone-gauge eigenstates.  This happens here, in so as to form two different individually taken distinct vibrational oscillations, that will here ripple along the Rarita Structure, in general, in so as to work at helping to form the gauge-metrical-based link between the activity of discrete quanta of energy permittivity, and, their directly associated gravitational particles, in so as to work at helping to form the interaction between discrete energy and its relationship with the fabric of space-time-bearing phenomenology.  Let us next consider that in this case, the helicity of the here given arbitrary gauge-action -- that is to be formed between the holonomic substrate of the two said Schwinger-Indices that have been mentioned in this case, were to then work to form an  ensuing Fourier-based activity -- that is of both the covariant, the codeterminable, and the codifferentiable delineation and distribution of the flow of the so-stated Schwinger-Indices -- to where this is happening, as such said vibrational-based indices are propagated along their correlative Rarita Structure eigenstates. This so-stated interaction of such a case, is to be bear a relatively proximal interface -- that is Yukawa in this case, in a supplemental-based tense of Ward polarization, over time, over the course of the directly pertinent so-eluded-to ensuing sequential series of group-related instantons.   On account of this genus of Ward-polarization,  the resultant Gliosis-based interface that is to end-up happening amongst the two here said Schwinger-Indices -- will be of a viable manner -- to where the said resulting wave-related interface, will be of a Gaussian-based nature, that will be of a covariant-based genus, that will then relate the two metrical gauge-actions, as two different Hamiltonian operators that will bear a Real Reimmanian-based spatial relationship between each other, to where this so-eluded-to Gliosis-based interaction will be of such a nature by which these will then act as being of the same universal setting.
I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.