Wednesday, June 22, 2016

What Helps To Form Modulae

Let us initially consider a given arbitrary orbifold eigenset -- when this is taken in terms of both its fractal modulus and its elastic modulus.  Determine what works at the substringular level, to help at both the formation of the respective given arbitrary orbifold eigenset's fractal modulus, as well as workling to help in the formation of its elastic modulus.  As an aside, let us think about the general Ward-Caucy-based conditions -- as to the relative Laplacian-based nature (which may also here be thought of as a tightly-knit Fourier-based set of conditions, that exist during the individually taken gauge-metrics during a group-related instanton) of those superstrings of discrete energy permittivity, as well as the conditions of those second-ordered light-cone-gauge eigenstates -- as these are to here exist during the tightly-knit Fourier-based conditions (or, the relatively loose correlative Laplacian-based nature), that are to exist over the self-same duration of group-related instanton, -- as the so-stated superstrings and their substringular counterparts work to form vibrational oscillations at their delineatory placements during BRST, which is during the same general state of that gauge-metrical activity that is to happen, as the said second-ordered light-cone-gauge eigenstates are "plucked" like a harp by their correlative gauge-boson eigenstates -- in so as to form the correlative Schwinger-Indices.  Both the vibrational oscillations of discrete energy permittivity, and the Fourier-related delineation and distribution of Schwinger-Indices -- are kinematically drawn along the directly corresponding Rarita Structure -- in so as to help to form that interdependent activity by which the Rarita Structure is to both form and implement the general proximal localized Ricci Field -- in so as to work to form those inter-connections that are to here exist between discrete quanta of energy and the activity of both gravitons anf gravitinos, over the course of a sequential series of group-related instantons.  For an orbifold eigsenset -- when there is a relatively high scalar amplitude of the immediate resultant of the vibrational oscillations of both superstrings and their correlative superstringular counterstrings, which are the quantum increments of discrete energy permittivity, upon the kinematic translation of wave-like activity along the Rarita Structure -- upon the correlative Ricci Field, then, this will then tend to be an indication as to the existence of a relatively high scalar amplitude of what would here tend to be the bearings of a discrete operation of a fractal modulus.  Yet, for an orbifold eigenset -- when there is a relatively high scalar amplitude of the immediate resultant of the vibrational oscillations of Schwinger-Indices, which would thereby be more pertinent to the workings of the correlative discrete energy impedance upon the kinematic translation of wave-like activity along the Rarita Structure upon the correlative Ricci Field, then, this will tend to be the bearings of a discrete operation of an elastic modulus.  The denser the activity of a given arbitrary tense of a Majorana-Weyl-Invariant-Mode tends to be -- the higher that the tendency is to that either the fractal modulus and/or the elastic modulus of an orbifold will tend to be, on account of this.  The less dense that the activity of a given arbitrary tense of a Majorana-Weyl-Invariant-Mode tends to be -- the lower that the tendency is to that either the fractal modulus and/or the elastic modulus tends to be.
Later, I will convey as to how both fractal and elastic modulae are formed, at more of a reverse "fractal" of physical phenomenology -- or, in other words, I will later convey as to how both fractal and elastic modulae are formed at more of a "macroscopic" level.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

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