Friday, August 23, 2013

The Second Part of the Fifth Session 5 of Course 14

From where I had left off before, with one-dimensional superstrings, the doubling up of mini-stringular segments from what would exist in the direct field of a light-cone-gauge eigenstate for two-dimensional superstrings of discrete energy permittivity -- works to double-up the Ward-Neumman boundary of the said light-cone-gauge eigenstate that works to connect the corresponding Planck-like phenomena that -- during the metrical course of BRST -- are just to the reverse-holomorphic side of the directly related one-dimensional superstrings of discrete energy permittivity, in such a manner in so as to form an optimum fractal modulus between the said Planck-like phenomena with their corresponding one-dimensional superstrings.  At the space-hole, some of the light-cone-gauge eigenstates almost begin to fray -- to just enough of an extent in order to temporarily form a small disconnection at the multiplicit relative Poincaires of the Bases of Light, in such a manner that works to allow for that form of order that is necessary for the multiplicit loci of those directly asociated substringular regions that are to be iterated in during the ensuing group instanton  to be able to flow without any unneccessary blockage -- so that phenomena may flow spontaneously under a condition of homotopy.  This works to allow for a total substringular connection to have an ability to bear no breakage in the topology of those superstrings that are here unfrayed.  Superstrings need to be arranged in the sequential and series arrangements that are necessarily based on vairous conditions, such as, what the substringular pattern was in the course of the prior iterations of group instanton, as well as being based on how the other superstrings of discrete energy permittivity, their counterstrings, the Planck-like phenomena, and the heterotic strings, were encoded to behave as during that Ultimon Flow eigenmetric that directly preceded the individual space-hole metric that happened right before the ensuing instanton-quaternionic-field-impulse-mode that is directly before a metric of group instanton.  I will continue with the suspense later!  Sincerely, Sam Roach.

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