The Ward-Neumman boundaries of a world-sheet is defined by two parallel Wilson Lines that are flush to each dimensional endpoint of delineation -- as to the furthest linearly-based mappable tracing that may be extrapolated in, in so as to mark each directoral basis as to the mapping of the region of where the directly corresponding ghost anomaly-based index may be tractable in one set locus, in so as to extrapolate the trajectory of the projection of any directly associated given arbitrary superstring -- that works to bear such a physical memory as to where and how the so-stated superstring had kinematically differentiated over time. As ghost anomalies form a basis as to where and how the world-sheets of superstrings had moved over time, there is a parallelapiped-based integration of world-sheets that are formed in general space-time fabric that may be multiplicitly utilized -- as to what may be termed of as a Klein Bottle. A Klein Bottle is composed of three sets of parallel Wilson Line-based world-sheet-like phenomena that work, in so as to bear a spatial operation that is kinematic and multispatially distributed and multispatially delineated in so as to work to allow for Kaeler-Metric eigenstates over time. The structural context of the Klein Bottle is known of as a Schotky Construction. The condition of World-Sheet-like phenomena that are parallel to one another is known of as the existence of orientafolds. The orientafolds that work to form the Schotky Construction are flush, as is according to the concept of Wilson-Lines. Wilson Lines are projections in the substringular that are literally flush, and thus do not bend as is according to the general curvature of space-time-fabric. The condition that the Schotky Construction bears orientafolds that are flush -- as is according to Wilson Lines -- is part of as to why the Klein Bottle is able to both shake superstrings into reattaining the fractal quantum indices of their discrete energy permittivity, as well as to shake Fadeev-Popov-Trace eigenstates into reattaining the fractal quantum indices of their discrete energy impedance. The static equilibrium of the indices that work to form the Schotky Construction is a given arbitrary condition of a conformal invariance of integrable orientafolds. Any given Klein Bottle eigenstate may be utilized, in so as to perform multiple eigenmetrics of Kaeler-Metric eigenstates, as long as the directly applicable Schotky Construction is not frayed.
I will continue with the suspense later! To Be Continued! Samuel Roach.
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