Scalar Amplitude Of Kahler-Based Quotients -- Correlative Intensity Of Wave-Tug

 Let us initially consider two different Noether-Based mass-bearing cohesive sets of discrete energy quanta, that are here to be of basically the same general nature. Both of these two different inferred individually taken "teams" of discrete energy, are here to be exhibiting the mappable-tracing, of a "congruent" tense of a Lagrangian-Based path, as this is here to be taken into consideration, over the durational course of a relatively brief covariant Fourier-Transformation, that is here to work to bear the span of the same sequential series of group-related instantons. (As the inferred covariant duration that is to be considered here, in which these two different inferred "teams" of energy, are here to have had worked to map-out their correlative Lagrangian-Based paths, is to be indicated by a monomial tense, of an evenly-gauged relativistic Hamiltonian eigenmetric.) Next; The kinematic motion of one of these two said cohesive sets of discrete energy quanta, is here to work to mathematically bear a greater scalar amplitude of a Kahler-Based quotient, than the other indicated cohesive set of discrete energy quanta, as this is here to be taken, over the covariant span of time, in which these two earlier inferred sets of discrete energy quanta, have worked to map-out their "congruent" individually taken Lagrangian-Based traces. As a result; that cohesive set of discrete energy quanta of the two, that is here to have worked to mathematically bear a greater scalar amplitude of a Kahler-Based quotient, -- in the process of working to map-out its correlative Lagrangian-based path, -- will consequently tend to work to bear a higher relativistic intensity of a wave-tug, upon its immediately external environment, than that other cohesive set of discrete energy quanta of the two, that was instead, to mathematically bear a lower scalar amplitude of a Kahler-Based quotient. I will continue with the suspense later! To Be Continued! Sincerely, SAMUEL DAVID ROACH.

Change In Vibrational Mode, And Homeomorphic Alteration In Impedance

 When the vibrational mode of a given arbitrary light-cone-gauge eigenstate, is to harmonically alter, over the course of a directly corresponding Fourier-Transformation, the directly associated increment of discrete energy impedance, will thereby consequently tend to change, in a homeomorphic manner. SAM. (1989).

More As To The Leverage Of The Higgs Action

The leverage of the Higgs Action, is caused primarily -- due to the leverage of the Fischler-Suskind Mechanism.  The general multiplicit condition of the Fischler-Suskind Mechanism, is comprised of by a correlative set of norm-state-projections, that work to bear a consequent orthogonal relationship -- that works to bear a wave-tug-related leveraging of ~6.25*10^18 (which is the reciprocal of the scalar magnitude of the smallest tense of discrete charge, which is ~1.6*10^(-19)Coulumbs) upon the correlative multiplicit Higgs Action eigenstate -- in so as to work to bring the activity of a Gliosis-related relationship, that is to ensue between discrete energy and the here directly corresponding multiplicit eigenstate of the holonomic substrate of the Klein Bottle, via the Kahler-Metric, in so that such a general tense of a Fourier-Transformation is here to be brought into the process of working to allow for the said multiplicit discrete quanta of energy to here to be re-attaining their fractals of discrete energy, in so as to work to allow for discrete quanta of energy to both persist and exist over time -- via such a relationship of a correlative general tense of a Gaussian Transformation.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Zero-Norm-State-Projections Causing Fujikawa Coupling

The general manner by which zero-norm-projections work to help at forming the general activity of the Fujikawa Coupling, is by the manner by which that the directly corresponding zero-norm-state-projection or projections -- that are here to act in so as to be bending the discrete quantum of kinetic energy permittivity in a hermitian manner, is acting in such a manner by which it is here to be arcing gradually although spontaneously in a hermitian manner -- via its correlative tense of a fractal of spin-orbital-momentum.  Here.  A given arbitrary set of one or more zero-norm-state-projections are to work to bear a wave-tug upon a discrete quantum of kinetic energy permittivity, that is to be subsequently released as the excess residual energy of an electron, in the form of a photon.  As such a said set of one or more zero-norm-state-projections are to bear a Gliosis-related Yukawa wave-tug -- upon the said discrete quantum of residual energy, the so-stated set of projections is then to work to bear a smoothly-curved torsioning upon the converting discrete quantum of energy -- in a manner that works to consequently smoothly bend the discrete kinetic energy that is then to be becoming discrete electromagnetic energy, in a manner that works to involve only as many changes in derivatives as the number of spatial dimensions that it is here to be traveling through, over its directly corresponding Fourier-Transformation.  It is the smooth translation of the fractal of spin-orbital-momentum -- that the here torsioning set of one or more zero-norm-state-projections are to be undergoing over time -- that is here to work to cause the consequent smooth translation of the hermitian bending of the here released kinetic energy of the corerlative electron, that is here to then ensue, in so as then to form a resultant photon (a photon is a discrete quantum of electromagnetic energy).
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

A Certain Aside As To Assymptotes

Let us consider an orbifold eigenset, that is moving into the general reverse-holomorphic direction -- in an assymptotic directorial-based manner, towards a plotting that may be mapped-out as being of a general relative y-based axion, -- to where this happens in such a manner, that may be described of as a cohomological index, that behaves as if it is moving as an eigenstate that is as well moving in a tangential manner, via a respective correlative Fourier-Transformation, that is initially being translated via an even manner of acceleration, over time.  Let us initially consider that one is dealing with a "real-to-'life'" relatively planar motion (as a figure of "speech"), that is basically moving in a strictly two-dimensional manner, as the said orbifold eigenset is to approach the so-stated relative y-based axion, in an assymptotic manner, over a sequential series of instantons.  Let us next consider, that at some point in time -- as the said orbifold eigenset is to then be relatively very close in proximal locus to the said mapped-out relative y-based axion, -- that the so-stated orbifold eigenset, that is to here be kinematic in displacement, via the so-eluded-to Fourier-Transformation, is to be tugged-across the Laplacian-based mapped-out y-based axion.  Since this general genus of a perturbation out of the initial assymptotic mode of motion, will be an alteration out of the general genus of the so-eluded-to approach -- that had initially been tending to get nearer and nearer to the plotted-out relative respective y-based axion -- in such a manner of which is to here be moving as is according to the so-stated initial even acceleration, over the initial so-eluded-to sequential series of instantons,  such a perturbation out of an assymptotic flow of the respective eigenindices of the said orbifold eigenset, will blatently work to cause a change in the initial rate of the acceleration of the said orbifold eigenset, -- to where such a genus of a kinematic-based perturbation will then work to cause a definite metrical-based Chern-Simons singularity.  Yet, since we are here to be initially discussing the actual versus the theoretical -- the actual approach of the so-stated orbifold eigenset that is towards the said Laplacian-based y-based axion, -- will work to bear, in reality, an external angular momentum -- that is to work to bear more of an abelian geometry of approach than a non-abelian geometry of approach, -- since the earlier said assymptotic motion of the said orbifold eigenset towards the so-stated Laplacian-based y-based axion, is to here, only be the physical result of what is simply an approximation of an assymptotic method of behavior.  (Nothing that is actually physical, is likely to just get more and more infinitely closer to any mapped-out axion, without ever to be able to spontaneously cross such a given arbitrary axion, no matter how long such an activity is to happen.  So, in reality, if such an approach is to be prolonged, such an orbifold eigenset will always tend to eventually alter from the theoretical assymptotic behavior, that has here been eluded-to.)  Based upon this just mentioned physical condition -- such a genus of a crossing of a Laplacian-based axion, will, in the "real world," not necessarily work to involve a Lagrangian-based Chern-Simons singularity.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Chern-Simons Singularities And Ghost-Based Inhibitors

Let us initially say that one is to have a metric-gauge-based Hamiltonian operator, that is to here be in the form of an orbifold eigenset that is to be translated via a Fourier Transformation -- in what is here the relative forward-holomorphic direction.  Let us next say that this given arbitrary respective holomorphic direction, is being observed of as to here be moving via a Lagrangian-based Hamiltonian operand -- that is of a relatively "straight" directorial-based path.  Let us next consider that there is to here be a sudden Lagrangian-based spike -- that is to happen to the said respective orbifold eigenset, that was, up until now, being propagated as a unitary Hamiltonian operator that was moving in a hermitian-based manner, in so as to bend in as many derivatives as the number of spatial dimensions that the so-stated metric-gauge-based eigenset was to here be moving through, as a parametric operator of a respective topological substrate.  Let us here say that the course of the activity that was here to be involved with the result of the said Lagrangian-based spike -- was to work to cause the said orbifold eigenset to then turn in the relative Njenhuis-to-forward-holomorphic direction -- at the cite of the so-eluded-to Lagrangian-based Chern-Simons singularity.  Part of what would tend to work to cause such a singularity, would be the motion of a ghost-based inhibitor, in the relative reverse-holomorphic direction to the initial motion of the orbifold eigenset of this given respective case, that would act in so as to work to form an initial Rayleigh scattering of the cohomological mappable-tracing of the projected trajectory of the ghost-based pattern that was being formed by the said orbifold eigenset.  Just as this so-eluded-to inhibitor is to begin in its Yukawa-based influence upon the said orbifold eigenset, this will then tend to pull the so-eluded-to cohesive set of superstrings, to then pull to what will here be the relative "left."  (This is if the forward-holomorphic direction is to here be considered as going relatively "straight.")
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.