During any one respective given arbitrary iteration of BRST, -- the more that a gauge-boson is to slide across the topological stratum of a correlative second-order light-cone-gauge eigenstate, instead of such a given arbitrary respective gauge-boson to act in so as to twitch upon the said second-order light-cone-gauge eigenstate of such a case -- the more that the resultant Schwinger-Index that is to then be formed as a tense of being a gravity wave, will then tend to work to bear a relatively higher period and a lower frequency -- than another Schwinger-Index that acts as a gravity wave, that is to instead to twitch upon such a said light-cone-gauge eigenstate to more of a scalar amplitude than it is to slide across such a second-order light-cone-gauge eigenstate. Furthermore, -- the more that a gauge-boson is to twitch upon the topological substrate of any said given arbitrary second-order light-cone-gauge eigenstate, instead of such a given arbitrary respective gauge-boson to act in so as to slide across the said second-order light-cone-gauge eigenstate -- the more that the resultant Schwinger-Index that is to then be formed as a tense of being a gravity wave, will then tend to bear a relatively higher frequency and a lower period -- than another Schwinger-Index that acts as a gravity wave, that is to instead to slide across the topological stratum of a such a correlative eigenstate to more of a scalar amplitude than it is to twitch upon such a respective eigenstate. The higher that the scalar amplitude of the correlative Polyakov Action eigenstate is -- the more that the correlative gauge-bosons will tend to bear a higher scalar amplitude of tending to slide upon the topological stratum of the correlative light-cone-gauge eigenstate. Furthermore -- the lower that the scalar amplitude of the correlative Polyakov Action eigenstate is -- the more that the correlative gauge-bosons will tend to bear a higher scalar amplitude of tending to twitch upon the said topological stratum instead of sliding upon it, -- during the course of any respective given arbitrary iteration of one duration of BRST.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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