Gauge-Bosons -- over the course of any given arbitrary respective iteration of BRST -- work to bear a general Laplacian-based condition, that is of the general state of initially being placed, in so as to ensue as to work at "plucking" the directly corresponding respective second-ordered light-cone-gauge eigenstates, in such a manner in so as to be distributed in such a delineaetion, in so as to work to bear a best-fit-curve to then being able to form the needed Schwinger-Indices, with the directly pertinent Ward-Caucy-based conditions that will here work to bear an optimum annharmonic pulsation with any immediately adjacent gauge-bosons that are to, as well, be able to form Schwinger-Indices -- with the physical condition of working here in a state of maximum rest-based capacity. This will then mean, that the respective given arbitrary gauge-bosons -- that are to here be directly affiliated with the Fourier-based translation of any of one given arbitrary respective iteration of BRST -- will then tend to be angled in a potential assortment, that may here work to bear a multifarious litany of Ward-Caucy-based angles. More later!
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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