Let us initially presume the potential general existence, of both the proximal local presence of E(5)XE(5) heterotic strings, And, the proximal local presence of E(3)XE(3) heterotic strings, as there is here to be kinematically exhibited in their display, in a certain tense of multiplicity, at various co-differentiable, co-determinable, covariant regions, that may potentially be mappable, in the general realm of the "arena" of superstring-related phenomenology. Let us next stipulate, the existence of a particular genus that is to be considered here, of an interaction, that is to be eminent in its existence, as taken between both of such earlier mentioned individually taken genre of heterotic string-related phenomenology, that I have started to discuss, in the case scenario that I am presenting right here. To "Cut To The Chase;" Let us say, that there is to be a spontaneous kinematic binary escalation, that is here to happen, amidst the prominent venue of the net wave-tug, that is here to tend to be primarily associated, with the dimensional-related pulsation, that is here to "emanate," from the durational kinematic transference, as taken over a directly corresponding Fourier-Related-Progression, that is here to be appertaining, to the eminently correlative spatial translation, of the directly associated Kahler-Related metric, that is here to be directly related, to the dual Lagrangian-Based motion, of the interdependent presence, of both the proximal local Ward-Cauchy-Related conditions, of the general inter-relationship, that is here to be present, as among the co-differentiable, co-determinable, and covariant general interaction, that is here to be kinematically latent, as between the resultant propagated topological sway, that is here to be interdependently driven, via the correlative wave-tug, that is here to be eminent in its direct association, that is here to be reductional in its correspondence, as this is here to be taken between the general interdependent gauged-action, that is here to be kinematically interactive, between both a given arbitrary E(5)XE(5) heterotic string, And, a given arbitrary E(3)XE(3) heterotic string. Let us next say, that one is to have a reductional genus of such a general situation, to where one is to have an inverted Yukawa Coupling, that is here to be situationally taken, between the Lagrangian-Based motion, that is here to be directly appertaining, to the two different and distinct individually taken propagated gauge-action-related wave-tug eigenstates, that are here to be of the earlier inferred escalation(s) -- of the earlier mentioned/inferred heterotic strings discussed here. To make things extra clear, the Inverse Yukawa Coupling, as mathematically taken, between the Binary Escalation most related to the motion of the given arbitrary respective E(5)XE(5) heterotic string, when in lieu with the Binary Escalation most related to the motion of the given arbitrary respective E(3)XE(3) heterotic string, will often, at times, be potentially capable, of working to exhibit the same general effect, as the topological wave-tug of the propagated kinematic gauged-action of an E(8)XE(8) heterotic string, may often work to exhibit. SAMUEL ROACH.
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