When one is to consider a one-dimensional superstring of discrete energy permittivity at BRST -- the directly corresponding first-ordered light-cone-gauge eigenstate that is correlative to the said superstring, works to bear five second-ordered light-cone-gauge eigenstates, that are here incorporated into the so-stated first-ordered light-cone-gauge eigenstate. Each of such so-eluded-to second-ordered light-cone-gauge eigenstates here will work to bear the Laplacian-based existence of having 120 correlative cites, during the correlative course of any respective given arbitrary iteration of BRST, where the directly corresponding gauge-bosons that are directly affiliated with the directly corresponding superstring will act upon the said second-ordered light in such a Gliosis-based manner at the Poincaire level, in so as to "pluck" the so-stated cites -- in so as to work to form the here necessary 600 third-ordered Schwinger-Indices, that are formed by the wave-functional activity of the correlative cite of discrete energy impedance, that are Yukawa to the eigenbase of the operational-based performance of the said correlative one-dimensional superstring of discrete energy permittivity, that is of any given arbitrary case in which such an implied source of discrete energy is unfrayed during the so-eluded course of the said iteration of BRST. Yet, if instead, one is here to consider a two-dimensional superstring of discrete energy permititivty at BRST -- the superstring will bear a first-ordered light-cone-gauge eigenstate that is comprised of ten second-ordered light-cone-gauge eigenstates, to where each of such individually taken second-ordered eigenstates will bear only 60 cites where the so-eluded-to third-ordered Schwinger-Indices will be formed -- in so that the overall first-ordered light-cone-gauge eigenstate of such a case will then, as well, work to bear a total of 600 third-ordered Schwinger-Indices, that are directly corresponding to the here correlative discrete quanta of energy.
If both of the here said general examples of first-ordered light-cone-gauge eigenstates are of a Yang-Mills light-cone-gauge topological-based construction -- there will initially have a consideration here of any of such so-eluded second-ordered light-cone-gauge eigenstates, that work to comprise the here so-mentioned first-ordered eigenstates, as bearing 60 Laplacian-based physically oriented sinusoidal-based oscillations that are existent at the general cite of the second-ordered light-cone-gauge eigenstates, that would here directly correspond to the Yukawa-based contact that is involved with the covariant differentiation of two-dimensional superstrings of discrete energy permittivity, in so as to be of the 60 cites per each of the second-ordered-light-cone-gauge eigenstates for the correlative gauge-bosons to be able to pluck the light-cone-gauge. When the correlative gauge-bosons work to "pluck" the here so-eluded-to sixty cites per second-ordered light-cone-gauge eigenstate of such a respective discrete quanta of energy -- the said plucking is initiated at the topological surface of the relative trough of each of the said sixty so-eluded-to Laplacian-based oscillations per second-ordered light-cone-gauge eigenstate, that are of the said Yang-Mills topology. Since two-dimensional superstrings work to bear 10 second-ordered light-cone-gauge eigenstates each, this would then involve a total of 600 of such cites, overall. This reverse-intuitive manner of plucking will then act as a springing mechanism, in so as to help to pull the so-stated correlative two-dimensional superstring of discrete energy permittivity into the generally unnoticed duration of Ultimon Flow. (Along with what I call the Imaginary Exchange of Real Residue.) Actually, it is such a springing effect -- that acts upon the so-eluded-to Clifford Expansion of the correlative light-cone-gauge -- that works to cause the here implied "woddle" of superstrings, that is pertinent to the so-stated Imaginary Exchange of Real Residue. The same general genus of activity happens with one-dimensional superstrings, that are of a Yang-Mills topology -- except that this will instead act upon the 120 cites of Laplacian-based oscillation per what would instead be the 120 cites where the correlative gauge-bosons would act upon the correlative loci of the so-stated second-ordered light-cone-gauge eigenstates (as before, though, this would involve a total of 600 cites overall (120*5 = 600)) -- in so as to cause the same general effect of a springing-based activity that is Gliosis to the topological surface of the light-cone-gauge at the Poincaire level -- in so as to help in the process of causing the Hamiltonian-based drive of putting superstrings into the generally unnoticed duration of the process of Ultimon Flow.
I will continue with the supsense later! To Be Continued! Sincerely, Sam Roach.
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