Operators And Group-Attractors, Part Six

Thus, conformally invariant sets of substringular phenomenology, like Majorana-Weyl-Invariant-Mode related masses -- tend to have more of a convergent set of relations.  Yet, covariant sets of substringular phenomenology -- that tend to diverge,  tend to be relatively more inexact and nonlinear in the expansion of their directly corresponding anti-chiral-based eigenindices, than covariant sets of substringular phenomenology that converge (to where the adjacent of such eigenindices will here be, instead, of an even-based chirality), as such said eigenindices are to tend to then be drawn into different respective substringular groupings.  However, first-ordered point particles, and waves that are delineated as norm-state-projections via the Fourier-based activity, that is here to be of the nature of certain given arbitrary differential geometries that are of such said first-ordered point particles, when such of these "building blocks" -- that are of the rudiments that work to form the composition of both superstrings and norm-state-projections -- when directed with the right angular momentum at the substringular level -- may often act as a fractal of an inductor of the conformal invariance for a set of one or more superstrings, and may often then act as a metrical-gauge-based Hamiltonian operator, that would work here to physically exist as an "integrating factor"-based holonomic substrate, or, in other words, as a catalyst, -- for the correlative Yukawa-based interaction of the directly corresponding group-attractors, to then act upon the topological surface of the directly corresponding specific given arbitrary discrete quanta of energy of such a respective case, in so as to bring this said discrete energy into a tense or a state of Majorana-Weyl-Invariance, at the Poincare level, that is to here be proximal localized at the Ward-Neumman/Ward-Caucy stratum that is to here be Gliossi in this case, to the holonomic substrate that is directly affiliated with the correlative discrete energy, that is being brought into a tense of conformal invariance.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.