Part 5 of An Aside to Differential Operators

When any given arbitrary substringular array is pulled equally between two axials, in the course of travelling throughout a unitary Minkowski-based Lagrangian, the manner of determining the appropriate extrapolation of the directly affiliated multiplets that are thence formed by the differential operation of the so-stated substringular array's motion through the so-eluded-t unit slope, is based upon the usage of the Slater Equation.  As an aside, the unit slope is based upon a 45 degree slope that is subtended equally between an arbitrary "x axis" and an arbitrary "y axis."  Now, let us say, instead, that one had a tense of a substringular phenomenology that was of a unitary Lagrangian that was subtended equally between one coniaxion and another coniaxion -- to where the angling that was directly involved with the motion of the so-stated substringular array, in the process of traveling through its pulsation of the Lagrangian of its directly corresponding Hamiltonian operand, was of a 45 degree-based geometric nature.  The resultant tense of the coefficient that is to be multiplied by the initial multiplet, in order to get the actual scalar amplitude of the wanted multiplet -- will here be based on the cosine or the sine of 45 degrees, or, 1/(the square-root of two).  This is if the destination of the so-eluded-to substringular array is at a parabollic-based end-point -- that is circled around the conicenter of the overall binary coniaxion, of this given arbitrary case scenario.  At the so-stated endpoint, the so-stated substringular array will tend to interact with a viable holonomic substrate, that works to bear a significant topological surface that is homotopically sound, in a Gliossi-based manner.  Likewise, from each individual Basis of Light, from the overall Bases of Light, this will, during the duration that is directly related to the "space-hole," cause the activity of the so-eluded-to traversing along the mappable tracing of the said Lagrangian, to work to incorporate a superstringular eigenbase -- for the correlative phenomenology that will here soon ensue to form superstrings of discrete energy permittivity -- to where a coniaxion-based center-state -- that will here work to involve the correlative eigenbase for the superstrings that are to be directly affiliated with that layer of reality that would here directly correspond to the layer of reality that is for each of the correlative Bases of Light that is not predominant -- if this is initially being in the same side of the dual-based world-tube, during the said duration that is here appertaining directly to the metric that is involved with the space-hole, or, if instead, the correlative eigenbase of superstrings of discrete energy permittiivity are of what is here the given arbitrary predominant layer of reality,  the majorization of the so-eluded-to eigenbase of what are to become superstrings of discrete energy permittivity are, during the "space-hole," located immediately in the cross-sectional part of  the dual world-tube construction of the same time-based eigenbase --that is of the same set of parallel universes.  To make things clearer, the predominant eigenbase of superstrings, in terms of the same layer of reality, will be located at the outer permutation of the same time-based dual-associated world-tube of the same set of parallel universes -- immediately to the cross-product-based locus, that is here just to the  exterior of the general center-state of its dual world-sheet of the same Basis of Light.