GUFT, Additional Addendum

When a superstring goes thru a Kaeler metric, the angling of the associated superstrings as a unit going into the given Klein bottle is 22 and a half degrees as subtended from a supplemental arc going in the direction of the ultimon's curvature pointing directly downward with the same ultimon curvature. One superstring usually undergoes 191 (96+95) iterations thru a Klein metric until it has completely regained the permittivity that it needs to be the energy that it's to be by the holomorphic/antiholomorphic shaking of the Kaeler metric. If the associated superstring still hasn't regained its permittivity after this, it will move reverse holomorphicly 95 iterative positions (one per core of BRST instantons), while then spinning at the same iterative locus for 80 iterations while then undergoing 10 spin-orbital/roll superconformal invariance modes at that locus. When this is the case, the associated superstring at this point will move into the core norm Ward boundaries of the Klein bottle directly transversally the 19th iteration hereafter this at the associated 22+(1/2) degree subtended angle. At this point, the first iteration of the next set of Kaeler metric iterations will happen to allow for the associated superstring to regain the permittivity that it needs to be the energy that it is to be. Each Klein bottle is 768 Planck Lengths long. Its exterior Neumman conditions consist of two normalized sets of orientifolds that allow the Klein bottle to be 384*768 Planck Lengths. This half cube's Neumman exterior boundaries consist of mini-string or superstringular fields that are hermitianly supplementally norm to form a fabric that is the equivalent of one Planck Length thick. This hermitianly supplementally norm field type exists at all four sides and the bottom of each Klein bottle. The interior of the Klein bottle consists of negative-norm first-ordered point particles that vibrate in the associated Schotky construction at 45 degrees from positive-norm first-ordered point particles. The difference between these negative norm states and positive norm states is that negative norm states initially go in the opposite direction of the Klein bottles And in the general transversal dirction in a forward moving time frame when the Klein bottle has absorbed superstrings, while positive norm states initially go in the same general transversal direction of the Klein bottle during a forward moving time-frame when superstrings are in the Klein bottle. In a backward moving time-frame, positive norm states go in the opposite general transversal direction of the Klein bottle, while negative norm states move in the same gereral transversal direction of the Klein bottle when superstrings are in the Klein bottle. The then associated fields of the norm states in the Klein bottle, these fields being mini-string subtended from the norm states that are interconnected in one fashion or another. So, the less metric-gauge that a superstring has as it goes into the Schotky construction, the more the skuperstring gets shuck to reattain permittivity in the form of metric-gauge. This "reverse proportionality" obeys a tangential Dirac function as a locus of superstrings changes the Jacobian eigenbasis of an orbifold or an orbifold eigenset thru a Clifford algebra that form a perturbative Fourie Transformation known as a Gaussian Transformation. When such a Gaussian Transformation alters the elasticity per hermicity of the associated light-cone-gauge eigenstates the associated light-cone-gauge eigenstates alters in abelian nature. This happens when norm conditions form a Yakawa Coupling with the associated superstrings.