Friday, June 20, 2014

Part Three of the Addendum Before Course 17

Superstrings of discrete energy permittivity do not start to go into a relatively discombobulated tense of covariant conditionality -- in terms of that directly corresponding multiplicit kinematic disposition that those first-ordered point particles, that work to comprise the so-eluded-to superstrings, bear, during the generally unnoticed duration-based portion of Ultimon Flow -- until the corresponding respective multiplicit Regge Action eigenstate is completed, in the interim that happens in-between BRST and the so-stated generally unnoticed duration -- that metrically exists in-between two given individual arbitrary instantons.  Within the the Ihbar so-eluded-to moment that happens after the so-stated multiplicit Regge Action eigenstate, all of the superstrings of discrete energy permittivity --  that work to comprise the given arbitrary layer of reality, or, tori-sector-range, will take aim to coalesce into a band of holonomic substrate-based phenomenology (that is either a relatively thick hoop-like band, or, a relatively thick strand-like band), that is put into a condition of what may be termed of as a "transition kernel."  This is the general Njenhuis-based gauge-metric, in which each partial association/dissociation integrand -- or, the quantific integration of all of the so-eluded-to superstrings, that work to form a group strand of phenomenology that still works to keep the directly associated differential characteristic differences that exist amongst each of the correlative superstrings that work to comprise the said tori-sector-range-phenomenology -- are put into the appropriate setting, in which there is a given arbitrary over-riding group attractor index quantifier, so-to-speak, that is kinematic upon the said tori-sector-range, in order to form a flux in the given needed group eigen-based transformation matrix.  As it is almost intuitive, the reverse-fractal basis of the correlative induction that is here formed will then be worked upon the so-eluded-to group strand of superstrings of discrete energy permittivity, that are here in transition -- in so as to work to form an antiderivative of a "conglomerate" group-pointal-flux.  Since this is a lot, I will continue with the suspense later!  To Be Continued, with the next cut to the chase!  Sincerely, Samuel David Roach.

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