A Little Bit About Substringular Couplings

What if a Yakawa Coupling that here existed in-between one set of superstrings had an even chirality, while the said Yakawa Coupling that also existed in-between another set of superstrings had an odd chirality, and, the two sets of superstrings that I just mentioned here in this given arbitrary case scenario were kinematically covariant?  The traits that I just described here by these two given sets of superstrings would have an assymetric J.  The compactification of the set of superstrings which had an even chirality would here propagate as a convergent series of holomorphic discharge, while, the compactification of the set of superstrings which had an odd chirality would here discharge Fock residue that would work to propagate as a divergent series holonomic eigenbasis.  As the two sets of superstrings that I just described interact as a reiterative variant operation, the assymetric-basis of their spin-orbital-interaction would here diverge as their angular momentum would simultaneously converge -- in a relativistical manner. As the spin of the two codifferentiating substringular traits that I just described work to polarize, in terms of their wave-tug delineations, the renormalization of their series output -- in terms of the consequent supplemental homotopic discharge -- this activity would here converge the local Poincaire distribution of the overall parity of the described given loci that is involved with the interaction of the two said traits.  The just mentioned two traits are here working to describe the interaction of the two said sets of superstrings that I have been describing in this given arbitrary case scenario.  The convergence that would then happen here would work to cause the given distribution of wave generators that are involved in this case to form a set of a fractal of covaliance. Such a "covaliance" would exist in-between the operational indices of those superstrings that worked to describe the two said traits.  These traits would here be eigen to the homostasis of a minimal variation of Ward-Caucy boundaries, when one is considering the desingularization of the corresponding substringular neighborhood fluctuations.  Such fluctuations would operationally allow for both the corresponding radial and transversal codifferentiation of a fixed matrical mode.  Such a mode would tend to not form critical cusps that would have a strong probablility of desolving upon an odd function of local kinematic transposition.  Once the corresponding transposition of the interactive decomposition that would result in the here mentioned case is encoded for by the substringular encoders -- while such a said transposition is iterated and reiterated in the same general process -- the corresponding Majorana-Weyl invariant anomalic substringulaar sway that would thence be formed by the related operation would spontaneously be nullified by the previous eigenaction.  The just mentioned activity would cause the corresponding Cassimer Invariant-mode to be physically integrated upon as a substringular fractal of a substrate, so that the resulting convergence of the insuing kinematic differential association may bear its correlative vibrational mode.  This would cause the creation of such a vibratory mode, of which would here produce eigenstates of Hamiltonian operation in terms of the resulting involvement.  This is so that the most directly inolved codifferentiable substringular trait that would be involved here would be able to then bear a Fourier-based condition of parametrically corresponding invariance.  I will continue with the suspence later!  Sincerley, Sam Roach.