Part Six of the First Session of Course 18

The said mechanism -- here being the Fischler-Suskind-Mechanism, happens via the activity of the multiplicit Klein Bottle, and, the so-stated Klein Bottle is put together in a manner that is termed of as the Schotky Construction.  Those superstrings that "tire" by their initial lack of their fractals of discrete energy permittivity -- as well as those directly corresponding Fadeev-Popov-Trace eigenstates that "tire" by their initial lack of their fractals of discrete energy impedance, go through a whole large process -- over a course of a sequential series of iterations of group instanton -- by entering the so-stated Klein Bottle, via a general genus of substringular activity or metric, that is known of as the Kaeler-Metric.  The Kaeler-Metric adds a certain degree of kinematic drive to the pulsation of the permittivity of superstrings that are then going through this general format of activity -- as well as the Kaeler-Metric adding a certain degree of kinematic drive to the pulsation of the impedance of the correlative Fadeev-Popov-Trace eigenstates that are then going through the general format of activity.  Such a general genus of special activity helps to allow for the Ricci Scalar to work at maintaining its needed relationships with the both the angular moduli, the spin-orbital moduli, as well as the transversal moduli, of the multivarious discrete units of energy -- that are portrayed by the kinematic activities of superstrings and their correlative Fadeev-Popov-Trace eigenstates.  A superstring is more likely to be in the process of undergoing a Noether-based flow, when it is undergoing the Kaeler-Metric.  Since any given arbitrary superstring and its directly associated substringular "entourage" will periodically enter the process of a Kaeler-Metric eigencondition, often, a tachyonic string will be undergoing a Kaeler-Metric eigenmetric -- yet in a manner in so that the cite of each ensuing iteration, whereupon the correlative substringular entities enter each ensuing stage of the here given arbitrary eigenstate of the Kaeler-Metric -- will here successively enter a different specific substringular locus per each of such stages of the said corresponding Kaeler-Metric, to where the eminent attributes of such a temporary constant alteration of specific locus are functionally indistinguishably different.  To be continued!  Sam.