Part Two of the Second Session of Course 18

When there is no relatively local Kaeler-Metric present for a given arbitrary set of adjacent superstrings, at a general locus in the substringular:  After BRST, the superstrings of discrete energy permittivity and their counterparts AS WELL as their correlative Fadeev-Popov-Trace eigenstates, which are of discrete energy impedance -- and their directly corresponding light-cone-gauge eigenstates, go into the correlative Regge Action eigenmetric, via the correlative Regge Slope, while then going into the generally unnoticed duration of Ultimon Flow.  When there is a relatively local Kaeler-Metric present for a given arbitrary set of adjacent superstrings, at a general locus in the substringular:  After BRST, the superstrings of discrete energy permittivity and their counterparts AS WELL as their correlative Fadeev-Popov-Trace eigenstates, which are of discrete energy impedance -- and their directly corresponding light-cone-gauge eigenstates, go into the directly correlative Klein Bottle eigenstate -- in so as to work to complete one iterative stage of the said Kaeler-Metric, at which point in gauge-metric, the so-stated substringular phenomena that enters the so-eluded-to Schotky Construction re-contracts back to the scalar magnitude of that condition that would be indicative of a completely Lorentz-Contracted condition.  After this entering into the said Klein Bottle eigenstate, the so-eluded-to substringular phenomena shakes eight times back-and-forth in so as to work to cause the shook phenomena to re-attain the needed fractals of respective discrete energy permittvity and its counterpart and discrete energy impedance and its counterpart -- while then going into the correlative Regge Action eigenmetric via the correlative Regge Slope, while then going into the generally unnoticed duration of Ultimon Flow.  This is enough to absorb for now!  Sincerely, Sam.