Let us here consider a discrete quanta of energy -- at one general locus, where the Polyakov Action is to be able to happen, -- during one specific iteration of BRST. During the Polyakov Action, at one respective given arbitrary locus -- the correlative superstring of discrete energy permittivity and its substringular counterpart, are decompactified to the inverse of as to the scalar magnitude of its directly pertinent Lorentz-Four-Contraction. As such a so-eluded-to Polyakov Action is happening -- both the Bette Action and the duration of the said iteration of BRST, are then happening simultaneously, through the vantage-point of a central conipoint. Any given arbitrary duration of BRST, is that activity that happens when a superstring of discrete energy permittivity is basically at a standstill -- aside from the activity that these said phenomenology go through in the process of both the said iterations of the Polyakov Action, the activity of the Bette Action, and the activity that is involved with the Imaginary Exchange of Real Residue. (This so-stated duration is the general metric that is to happen over a majority of any directly correlative iteration of instanton.) As a refresher to my readers -- the Imaginary Exchange of Real Residue is involved with that activity in which the directly corresponding counterstring of discrete energy permittivity is to initially sway in the relative forward-holomorphic direction, at a subtension that is initiated in a spot that is relatively proximal to the relatively reverse-norm-to-holomorphic position of the directly affiliated counterstring, while this said genus of metric works to bear an equal and opposite reaction of then working to bear a toplogical sway of the directly corresponding superstring of discrete energy permittivity -- that is pulled into the here relatively reverse-holomorphic direction, at a subtension that is initiated in a spot that is relatively proximal to the relatively reverse-norm-to-holomorphic position of the directly affiliated so-stated superstring of discrete energy permittivity. Such a so-eluded-to topological sway is like a "woddle" of the overall discrete quanta of energy permittivity. (The said superstring is more pertinent to the particle-based nature of such, and, the said counterstring is more pertinent to the wave-function-based nature of such.) As the earlier mentioned respective given arbitrary superstring that is undergoing a metric of a pertinent iteration of BRST -- at a relatively set substringular locus -- the gauge-bosons act in so as to "pluck" their directly correlative cites, at the respective given second-order light-cone-gauge eigenstates. This is able to happen, because the here applicable topological Yukawa inter-relationship -- that would here exist in-between the cites as to where upon the second-order light-cone-gauge is to be plucked, & the Ward-Caucy bounds of the correlative said gauge-bosons, that are to do the said plucking of the said second-order eigenstates of the wave-functionability of discrete energy impedance, is not of a manner that would OTHERWISE be of a Glioisis-based homotopic bearing tangency -- during the so-stated general activity of the said "plucking" that is to here happen over the individually taken successive series of the correlative iterations of BRST. This means, that -- even though the homotopic condition of the substringular interconnections that exist among all unfrayed superstrings tend to work to bear a condition of a general state of Cassimer Invariance -- the gauge-bosons of the substringular are most Gliosis in interconnection with that topology that is of the multiplicit Rarita Structure eigenstates, that are off of the relative Real Reimmanian Plane, -- to where, the so-implied homotopic indices that are directly tied upon the here so-stated gauge-bosons will then tend to be of a Njenhuis-based nature to the Sterling-based field of the relative field-density of the directly correlative discrete quanta of energy, that is of such a case. So, this leads to allow for the condition, that this just mentioned state of affairs -- that is of the inter-relationship between gauge-bosons and the directly corresponding second-order light-cone-gauge eigenstates, will then here work to tend to bear a higher and spontaneous scalar magnitude, that is of the freeing-up of room, that is proximal to the Poincaire level as to the here relative positioning of these said interacting phenomenology, to where the correlative plucking that I have here described, may be able to tend to happen without any perturbative unwanted torsioning of the core-field-density of the here directly corresponding and local discrete quanta of energy, that are most Yukawa to the here said case scenario.
I will continue with the suspense later! To Be Continued! Sincerely, Sam Roach.
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