The physical composition of any respective given arbitrary Klein Bottle eigenstate, is comprised of as the following: Two widths that act as orientifolds -- that are traversed in a Laplacian-based manner across the length of the said Schotky Construction. Two thicknessses that act as orientifolds -- that are traversed across the width of the said Schotky Construction. And, a relative "bottom" (at the relative norm-to-reverse-holomorphic positioning), that is situated in so as to bear both a Laplacian-based traversing across both the length and the thickness of the so-stated genus that works to comprise the said Schotky Construction. The length of the Schotky Construction is four Planck Lengths. The width of the Schotky Construction is two Planck Lengths. The thickness of the Schotky Constuction is one Planck Length. The relative "top", or, in other words, the relative norm-to-holomorphic positioning of the said Construction is left open -- in so as to allow for both superstrings of discrete energy permittivity and their counterparts & in so as to allow for the correlative Fadeev-Popov-Trace eigenstates and their directly affiliated light-cone-gauge eigenstates to be able to enter the so-eluded-to respective given arbitrary Klein Bottle eigenstates, to be able to undergo the needed directly corresponding Kaeler-Metric eigenmetrics. Orientifolds are topological "sheet-like" holonomic substrate that are both situated in a parallel manner, as well as being positioned as is according to a Wilson-based linearity. A Wilson Line is a supplemental physical condition that is Yakawa to a directly corresponding substringular situation. You may now be wondering how the multiplicit Klein Bottle eigenstate is physically able to maintain the so-eluded-to Wilson linearity of its directly corresponding Schotky Construction. I will explain a little bit about this here. The means as to how the Schotky Construction is able to maintain its ability to be able to comprise the multiplicit Klein Bottle eigenstate, is the activity that is involved with the process of the conformal invariant condition of the correlative Fischler-Suskind-Mechanism. When the correlative Gaussian parameters that interplay upon a Klein Bottle eigenstate, differentiate in a kinematic manner upon the holonomic substrate of a discrete composition of the Schotky Construction, this works to alter the renormalization of the directly involved Jacobian eigenbase -- that is affliated with those conditions that work to initiate a Gaussian Transformation upon a respective given arbitrary set of superstrings -- then, the correlative Schotky Construction is temporarily caused to diverge -- in so as to meet the metrically enacted upon norm-conditions, which works to cause the correlative given arbitrary respective Klein Bottle eigenstate of an individual case to move in an increased manner toward a more primed geometric location, over the duration of a relatively transient number of group-related instantons.
I will continue with the suspense later! To Be Continued! Sincerely, Sam Roach.
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