Part Two of the Interim In-Between Sessions 7 and 8 of Course 18

If the proximal encodement of the superstrings of the scenario that we have been dealing with here is maintained over the sequential series of group instantons of the so-stated group-related metric, then, the general condition of the first-ordered point particles that have worked here -- in so as to help to cause the directly corresponding superstrings to be of such a conformally invariant nature, in so as to be near each other, in such a tense of a Majorana-Weyl invariant nature, will work to allow for the so-stated point particles to bear  of a relatively proximal nature to a certain extent as well.  This is when this is taken in consideration of their correlative neighborhoods in the globally distinguishable.  Yet, if the directly corresponding reverse-fractaled tense of the electrostatic nature that is propagated from the directly corroberative superstrings will then here bear a divergent tense of residual homotopic Hodge-based indices, over the so-eluded-to sequential series of group instantons that work to correspond to the time in which the correlative superstrings are here being associated -- in the course of the so-eluded-to tense of superconformal invariance of this corroberative scenario, then, there will here be at least some sort of alteration in the localization of some of the superstrings that were directly associated with the so-stated group metric of this general scenario.  Yet, if the correlative superstrings are to remain relatively unchanged locally after each iteration of group instanton -- when in terms of their respective codeterminable codifferentiation, over each corresponding discrete increment of time that is to be metrically mapped-out in so as to work to help determine the genus of the specific tense of superconformal invariance that is involved here, then, the index of the prior tense of the respective perturbation of electrostatic differentiation is to be nullified in consideration.  The higher the Dirac factor is in terms of the non-local substringular phenomena -- that is to bear an exterial spin-orbital and/or a transversel effect upon the more directly involved interial-based phenomena, of such a format of a scenario, in spite of the degree and/or the level of the scalar magnitude of the physical separation that may exist here, the more assymetrical that the correlative superstirngs will tend to covariantly be propagated through in a kinematic manner -- relative to one another, over the so-eluded-to group metric -- when such a tendency is considered time-wise through a coniaxion that is centered at the convergent-based loci of the directly corresponding Fadeev-Popov-Trace eigenstates.
I will conclude with this interim later! To Be Continued!  Sam Roach.