What I am about to talk about first, is most related to substringular impedance -- so read carefully -- and "hold onto your hats!" The higher that the scalar amplitude of the Polyakov Action eigenstate is, the more mini-stringular segmentation that there will tend to be -- that is fed into the proximal locus of the directly corresponding first-order light-cone-gauge eigenstate. The more mini-stringular segmentation that there will be, that is fed into the proximal locus of the directly corresponding first-order light-cone-gauge eigenstate -- the more mini-stringular segmentation that there will tend to be, that is fed into the correlative proximal local second-order light-cone-gauge eigenstates, that are here to have worked to comprise the earlier mentioned first-order light-cone-gauge eigenstate. This relative insurgence of mini-stringular segmentation, will then tend to work at causing a relative insurgence of impedance-based interconenctive mini-stringular eigenindices -- of which will then tend to work to cause a relative increase in the scalar amplitude of the proximal local impedance-based covariant field eigenindices -- that will then tend to be proximal at the here relatively adjacent substringular neighborhood. Here is an example, in so as to work to elaborate at what I mean by this. Mini-Stringular segmentation is what works to inter-connect Ward-Cauchy-based substringular phenomenology, as well as the condition that mini-stringular segmentation is what works to form both substringular fields and the general basis of homotopy. Such said segmentation is what works to hold the unfrayed quanta of energy in the space-time-continuum together, per each successive iteration of group-related instanton. The more of a "Hodge-Index" that one is to relatively bear, as to the scalar magnitude of the degree of the mini-stringular segmentation, that is then to be present -- the more likely that there is to be a higher scalar magnitude as to both the number of mini-stringular inter-connections, as well as the number of inter-connective field eigenindices -- that may exist here, to be utilized in so as to then to work to bear a Yukawa Coupling with that general stratum, that is here to be most directly associated with such an increase in mini-stringular segmentation. Thence -- when the Lorentz-Four-Contraction that is most directly associated with a phenomenon is low, and its consequent Polyakov Action, is then to be high -- then, its consequent light-cone-gauge eigenstate, and thus the directly corresponding wave-related tense of substringular impedance, will then tend to bear a higher stability of homotopic residue. This will then tend to be the inverse as to what will happen to the correlative discrete quantum of energy permittivity. This will then tend to, instead, to work to decrease the field-interconnection-based eigenindices, in so as to work to bear a lower stability of homotopic residue -- that would otherwise work for superstrings of discrete energy permittivity. "Superstrings," in my model, may be generally typified as being superstrings of discrete energy permittivity.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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