Reason For Adjacent Phenomena Orphoganal, Part One

Let us initially reflect upon a point that I had made in the past -- while then, working to develop the ideas that I am about to present, into what will amount to a hightened potential understanding of the modus operandus of the substringular realm.  Here it goes.  Any two discrete quanta of energy that are to here be immediately adjacent to each other -- as being two discrete physical phenomenology of topological substrate -- must be geometrically arranged into both a covariant, a codeterminable, and in a codifferentiable manner, by which, at a theoretical Laplacian-based "snapshot," that could be taken over the course of the exact moment that exists right before the proximal localized Polyakov Action eigenstate, that is at the Poincare level to the general locus of two given superstrings in the substringular level, that are right next to each other, to where the holonomic substrate of the one discrete increment of physical energy is to bear a Real Reimmanian tense of orphoganation to the holonomic substrate of the other discrete increment of physical energy, that is of a Real Reimmanian tense -- in as long as both of the so-eluded-to discrete quanta of energy are of the same universal setting.  The reason as to why this tends to be the case, -- is because, since a superstring of discrete energy permittivity tends to exist as either a two-dimensional  or as a one-dimensional fabric-formed holonomic substrate, that is pushed through what will here tend to be anywhere in the "arena" of being a Hamiltonian operand that is to exist as being a substrate of being from between four to twelve spatial dimensions -- per each discrete increment of group-related instanton -- to where this tendency, as to what has to take place, in order for there to be any viable interaction between the so-eluded-to eigenstates of topological-based holonomic substrate, that is to bear enough of an abelian geometry, in order for the dual Hamiltonian-based action to be eigen to both superstrings in a Gaussian manner that is Yukawa in a Real Reimmanian manner over a sequential series of instantons, -- then, there will here tend to be the need for a coniaxion-based cross-section of the topological core-field-density of the one discrete quantum of energy upon the other discrete quantum of energy, over a relatively transient but discrete group-metric, -- that will here be of an integrated Fourier Transformation, that will tend to be piece-wise continuous, over a discrete duration of time.  I will continue with the suspense later! To Be Continued!  Samuel David Roach.