Schwinger-Indices And A Common Node

Let us initially consider two different given arbitrary respective Schwinger-Indices -- of which are to here be in the process of being propagated as gravity waves, across the Hamiltonian operand of two different distinct segments of mini-stringular topological stratum -- over the course of a relatively transient sequential series of group-related instantons.  Let us next consider, that the two distinct so-eluded-to wave modulae -- that are to here be transmitted across a discrete Lagrangian path -- are to work to bear two different distinct and respective oscillation-based patterns, over the so-eluded-to group-metric, -- to where, the resultant dual vibrational oscillations, are to here be working to form a set of two general disturbances in space, of which are angled toward a common node-based singularity in space, due to the condition that the directly corresponding holonomic substrate of the two so-eluded-to distinct segments of mini-stringular topological stratum, are to here be subtended from one another in such a manner, in so as to form a binding point, that is positioned in a Laplacian-based manner, that is positioned further along in the relative forward holomorphic direction from the initial dual disturbance in space, by which the two said respective Schwinger-Indices of this case had been initially propagated towards a common node in time and space.  When one is to, as well, work to consider both the manner of the angling of the two respective mini-stringular segmentations that are to be vibrating towards one another, along with the Ward-Caucy conditions of the eigenfunction-based Hamiltonian operation of the performance of the correlative Schwinger-Indices, as these are being oscillated as a "domino-effect" towards the so-stated common node -- that is to here be positioned in a Laplacian manner at a spot that is "further-up" in the relative forward holomorphic direction, then, the integration of these eigen-related conditions, when this set of conditions is coupled with the parameter-based conditions as to the Gaussian-based additions that are to be made Yukawa by the coupling of the two so-eluded-to wave modulae, that are to here be coming together, this will then work to help at working to form the resultant eigenstate of the then singularized discrete unitary Schwinger-Index, that is to then be of one integrative vibrational oscillation, that is to then act as one discrete metrical-gauge-based Hamiltonian operator, that is to then act as a gravity wave-based pattern, that is to here be imbued upon the topological stratum of one inter-bound eigenstate of mini-stringular segmentation.  I will continue with the suspense later!  To Be Continued!
Sincerely, Samuel David Roach.