Schwinger-Indices And Mini-Stringular Segmentation

Let us initially consider one given arbitrary relatively compactified "collage" of mini-stringular segmentation -- that is to here be vibrating as one discrete metrical-gauge-based Hamiltonian operator, in which that specific example of an initial disturbance in space, that had must been enacted upon the so-stated integrative conglomeration of mini-stringular segmentation, in so as to help in working to form a tense of that general genus of a Ward-Caucy-based vibrational oscillation, that could be described of as being gravity waves in such a case, may then be thought of as a propagation of Schwinger-Indices, that are to here, ripple -- from the time-based locus as to when the so-eluded-to covariant, codifferentiable, and codeterminable "collage" of mini-stringular segmentation had absorbed the earlier mentioned disturbance in space, in a Fourier-based manner as a kinematic Hamiltonian operand, that as well will here act as a Hamiltonian operator, due to the here exasperative fluctuation of wave-based eigenstates, that are to here be perturbated, due to the metrical activity of the initial said disturbance -- up to the latter positioned holonomic substrate, that in of that ensuing Lagrangian-based Hamiltonian operand, in which that holonomic substrate-based phenomenology that is to here act as the then remaining gauge-attraction eigenindices, that are to here be in the process of being used-up or elliminated, via the process of these said eigenindices being put into such a Ward-Caucy-based condition, by which these will be allowed to then run-out their course, by such eigenindices to have then been fully degenenerated by being depreciated of their directly corresponding fractals of the eigenindices of the here correlative gauge-based attraction, that is to here be directly related to that initial disturbance in space, that had acted as those Schwinger-Indices that had behaved as the gravity waves that were initially formed by the "plucking" of the here correlative light-cone-gauge eigenstates by their correlative gauge-boson eigenstates, that had happened to the directly corresponding Rarita Structure, at an earlier tense of a gauge-based metric.  I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.