Monday, December 29, 2014

Part One of an Interim In-Between Sessions 7 and 8 of Course 18

I am about to explain a certain genus of parity interactions of eigenstates, that are in reference to superstrings that are formed in an alternating sequential manner, in order for the correlative superstrings to be able to release wave homotopy that would here work to encode for a specific unique superstringular trait.  Let us initially say that one was to here consider ten superstrings of discrete energy permittivity that will have, over a correlative group metric, been reiterating, per directly corresponding respective group instanton, in their correlative substringular neighborhoods.  Let us now here consider that, after about one quadrilion successive group-related instantons, the sequential eigenmetric of the ten here mentioned superstrings of this particular case -- although maintaining their relative proximal encodement -- starts to differentiate kinematically in a different Majorana-Weyl covariant-based mode, when one is to compare the Hamiltonian-based codetterinable interactions of each of the ten so-stated superstrings, in relation to one another, as both a substringular index of their individual substringular behavior when taken individually and also when taken as a substringular index of their group substringualr behavior when taken as a group that acts as an orbifold. This alteration in both the individual activity of the ten component superstrings of the just eluded-to orbifold, and in the activity of the said orbifold as a whole, will work to form a tense of a divergent singularity in the encodement of its resultant integrative Hodge-based Hamiltonian operation, that will work to cause the homotopic residue that is then here formed by the so-eluded-to alteration in the genus of the activity of the so-eluded-to orbifold to change at least one globally distinguishable overall trait -- that will then be able to be detectable by the domino effect of this orbifold -- when the result of such a perturbative reaction is inversely traced into a corresponding extrapolation that may be observable in a here correlative reverse-fractaled chain of events.
I will continue with the second part of this interim later! To Be Continued!  Sam Roach.

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