Expansive Inversion Of Dispersed Homotopic Residue

The expansion rate of re-calibrated harmonic Chern-Simons Invariant gauge-actions, may often tend to be eminently associated, with the rate of charge generation. 

Whereas; The expansive inversion of dispersed homotopic residue, may often tend to be eminently associated, with a genus of the perturbation of space-time-fabric, that works to help facilitate the general process, of charge generation. 

I WILL CONTINUE WITH THE SUSPENSE LATER! SINCERELY, SAMUEL ROACH.(1989).

A given arbitrary tense, of a physical display of Tesla-Related Energy, may often tend to exhibit, a kinematically propagated tense, of inter-dispersively covariant, net kinetically transferred fields, that are eminently associated, with Dolbeault-Related cohomology. 

The more heuristically gauged the pulsation, the more succinct the motion. The more metrically gauged the pulsation, the more resolute the motion.  

The more resolute behavior, that the Fourier-Related-Progression, of an eminently associated Kahler Hamiltonian Topological Manifold, is to endeavor exhibit, the more “pressure-related thrust,” that the Lagrangian-Based Drive, of such a “team” of discrete energy eigenstates, may often tend to spontaneously work to physically express, in the general process, of its kinetically transferred kinematic propagation. Furthermore; The more succinct behavior, that the Fourier-Related-Progression, of an eminently associated Kahler Hamiltonian Topological Manifold, is to endeavor to exhibit, the more “puncture-related thrust,” that the Lagrangian-Based Drive, of such a “team” of discrete energy eigenstates, may often tend to spontaneously work to express, in the general process, of its kinetically transferred kinematic propagation. 

The stronger that the Non Abelian wave-tug is to be, the stronger that its spontaneously associated propagation-related enfoldment, will consequently tend to be. 

Furthermore; The stronger that the Abelian wave-tug is to be, the stronger that its spontaneously associated propagation-related warping, will consequently tend to be. 

Whenever a team of mass-bearing discrete energy eigenstates, is to change in its speed and/or direction, relative to light, its i*PI(Del)Action is thence to spontaneously become effectual. Likewise; Whenever a team of mass-bearing discrete energy eigenstates, is to change in its speed and/ or direction, relative to light, its eminently corroborative net Chern-Simons Invariant gauge Action eigenstate, will spontaneously tend to re-calibrate. Therefore; Whenever Chern-Simons Invariant gauge-actions are to re-calibrate, its eminently corroborative i*PI(Del)Action, will spontaneously tend to bear viably effectual. 

Re-Calibrated Chern-Simons Invariant Gauge-Actions

 The Expansion rate of re-calibrated Chern-Simons Invariant gauge-actions, may often tend to be eminently associated, with the expansive inversion, of dispersed homotopic residue. SAMUEL. 

Electromotive Charge tends to be eminently associated with cohesion, stability, and physical ordering. 

Moreover; Physical Entropy tends to be eminently associated with incoherence, instability, and physical chaos. 

The re-calibration of Chern-Simons Invariants (which are only kept “invariant” when the corroborative rate and direction are held constant), at one spot at one stage, can either be harmonic, or it can be anharmonic. The harmonic re-calibration of Chern-Simons Invariants works to form charge — thereby tending to move in the direction of order. Whereas; The anharmonic re-calibration of Chern-Simons Invariants works to form entropy — thereby tending to move in the direction of chaos. That’s why this topic is SO important!

Gyrating flying saucers, tend to move in the general direction, in which the net Fourier-Related-Progression is to peak, at the proximal local tightly-knit region, at which the holomorphic zero pole of the homotopic transfer is to be induced into, as the implicit team of discrete energy moves. 

Cohesive Fourier-Related Systems, will often tend to be hermitian; &; Dispersive Fourier-Related Systems, will often tend to be entropic. 

A set of interdependent physical frequencies, that operate to perform a common function, will often tend to be eminently corroborative, with a hermitian Fourier-Related-Progression. 

A set of interdependent physical frequencies, that operate to perform a set of relatively unrelated functions, will often tend to be eminently corroborative, with an entropic Fourier-Related-Progression. 

The physical incursion of sound, upon a progressively delineated, kinematically propagated, interdependent set of physical frequencies, may often tend to enhance the general characteristics, of the spontaneous potential resultant, of a hermitian Fourier-Related-Progression. 

The physical incursion of heat energy, upon a progressively delineated, kinematically propagated, interdependent set of physical frequencies, may often tend to enhance the general characteristics, of the spontaneous potential resultant, of an entropic Fourier-Related-Progression. 

Isometric molecular vibration, often tends to facilitate the formation of sound, thereby potentially enhancing the proximal local tendency, of hermitian wave progression. 

Asymmetric molecular vibration, often tends to facilitate the formation of heat, thereby potentially enhancing the proximal local tendency, of entropic wave progression. 

Heuristic Coupling Of Thought With Power

 The multiplicity of the heuristic coupling of thought with power, often tends to spontaneously facilitate, the rate at which force is to be physically applied, upon its environment. SAMUEL ROACH. (1989).

High Frequency Thought Waves -- Relatively Quick Transference

 A given arbitrary Noether-Based thought wave, that is here to be of a relatively low wavelength, may often tend to work to bear a relatively high frequency, to where, if such a respective thought wave is here to be incurred upon, by a recursively covariant isotropically stable kinematic source, of gauge-action-related phenomenology, in such a manner, to where the resultant kinematic transversally applied wave-tug, is here to work to bear a monomial tense of a scalar amplitude, this will often tend to consequently work, to cause the said thought wave in question here, to be physically transferred to its transversally delineated destination, at a relatively higher rate of velocity, than it otherwise would. TO BE CONTINUED! SAM.

Chern-Simons Invariance -- Gauge-Invariance

 A given arbitrary discrete quantum of energy, is to tend to work to bear the general proximal local  characteristic, of what may here to be considered as being the Ward-Cauchy-related condition of Chern-Simon Invariance, -- when such a said discrete quantum of energy, is here to also work to bear the general proximal local characteristic, of what may here to be considered, as being the Ward-Cauchy-related condition of gauge-invariance. The general physical characteristic of Chern-Simons Invariance, is only of a heuristic manner of exemplification, when the directly associated discrete quantum of energy, is to be in the process of displaying both a constant rate of spatial translation,And, a constant direction of projected trajectory, as this is here to be taken, When in its covariant relationship with the motion of electromagnetic energy. Likewise; the general physical characteristic of Gauge-Invariance, is only of a heuristic manner of exemplification, when the directly associated discrete quantum of energy, is to be in the process of displaying both a constant rate of spatial translation, And, a constant direction of projected trajectory, as this is here to be taken, When in its covariant relationship with the motion of electromagnetic energy. So; whenever a Noether-based discrete quantum of energy, is to alter in either its speed and/or in its direction, in its relationship with electromagnetic energy, -- such a said quantum of energy, is then to alter out of the general Ward-Cauchy condition of gauge-invariance, -- to where its initial condition of Chern-Simons Invariance, is thereby to become variant in the process. To conclude: Both the physical condition of Gauge-Invariance, And, the physical condition of Chern-Simons Invariance, are only heuristically as such, as a given arbitrary directly corresponding cohesive set of discrete energy quantum, that is here to be in the process of being taken into consideration, is to be maintaining both the same rate of speed, And, a constant direction of its projected trajectory, when this is here to be considered, in its relation to the motion of electromagnetic energy. I will continued with the suspense later! To Be Continued! Sincerely, Samuel David Roach. (1989).

The Next Part; As To A Derivation Of, "Homotopic Residue"

 Initially, as a refresher; when a mass-bearing cohesive set of discrete energy quanta, is to change in its direction and/or in its rate of motion, when in relation to the motion or electromagnetic energy, the correlative Specifics, as to what the Chern-Simons Invariants are actually to be working to consequently express, will thereby tend to go into a state of alteration (perturbation). When Chern-Simons Invariants, are to go into a state of recursive perturbation, (as this is here to be appertaining, to the implied general physical conditions, of "excited" mass-bearing cohesive sets of discrete energy quanta), -- this will often tend, at least for some sort of a "Poincare level," to work to form a certain tense or manner, of what I term of as being the general physical attribute, of "cohomology-related dispensation." This said "cohomology-related dispensation," is consequently to tend to result, in having the general characteristic, of working to reverse-fractal, into what to us, is to tend to be the existence of electrodynamic charge. To Be Continued! Sincerely, SAMEUL ROACH. 

Permeability And Recursively Smooth Ricci Flow

 When one is to have a mass-bearing cohesive set of discrete energy quanta, that is here to be spatially transferred -- at both an even transversal rate and at an even rotational rate, -- the greater the electrodynamic permeability, the more recursively smooth that the correlative Ricci Flow is to tend to be. Sincerely, SAM ROACH.

Majorana-Weyl-Invariant-Spinors

Even though any given arbitrary Majorana-Weyl-Invariant-Spinor, is to tend to bear a transversal manner of superconformal invariance -- at an internal reference-frame, -- since the direction of its correlative angular momentum is to constantly be altering, over time, -- such a said respective general tense of a constantly spinning phenomenon, is to tend to constantly bear a manner, of a directly associated radial acceleration (since, to paraphrase things, an acceleration is a change in either the rate and/or in the direction of any moving phenomenon). To Be Continued! Sincerely, Samuel David Roach.

Adjacent Spinning Mass-Bearing Orbifold Eigensets

When two different adjacent given arbitrary mass-bearing orbifold eigensets, are here to be spinning at a relatively high rate -- these will each tend to need to bear a covariant asymmetric spin in relation to one another, -- in order to not infringe upon each other's space.  This is why adjacent electrons tend to bear a covariant asymmetric spin, in relation to one another, again, in so as to not infringe upon each other's space.  This specific general example that I just mentioned, in respect to the nature of the spin of adjacent electrons, is commonly known of as being the general gist of the "Pauli-Exclusion Principle."  I will continue the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Orbifold Eigenstate Pulsation And Rate Of Transference

The quicker that any given arbitrary orbifold eigenstate is transferred in its delineation through space over time, the quicker that its rate of pulsation will consequently tend to be.  Next; let's consider two different orbifold eigenstates, that are both to be pulsating at the same covariant rate. Next; let's theoretically consider, in this particular case, that both of the here stated orbifold eigensets, are to be effected by the same scalar amplitude of substringular pressurized vacuum. Let's next say, that the individually taken superstrings of discrete energy permittivity, that work to comprise one of these two said orbifold eigensets, are to be vibrating at a quicker rate, -- than the individually taken superstrings of discrete energy permittivity, that work to comprise the other of the two said orbifold eigensets.  Let's next say, that both of these here stated orbifold eigensets, are to work to bear both the same number of superstrings of discrete energy permittivity, over the course of their spatial transference of delineation. Both of such here mentioned orbifold eigensets, are also to work to bear the same density. The orbifold eigenset of this particular case, that is here to work to bear the proximal local presence of those inferred superstrings of discrete energy permittivity, that are here to be vibrating at a quicker rate, -- will consequently tend to bear a greater fractal modulus -- than the other of the two mentioned orbifold eigensets. Sam Roach.

Chern-Simons Invariants

Let us initially consider two different orbifold eigensets, that are here to be moving in a covariant manner -- over an evenly-gauged Hamiltonian eigenmetric.  Both orbifold eigensets are here to be moving at both the same transversal rate, And, at the same radial rate, -- in their relation to light.  Furthermore; both orbifold eigensets are also here to work to bear both the same angular momentum And the same spin-orbital momentum, -- over the same earlier inferred evenly-gauged Hamiltonian eigenmetric.  Otherwise, both of these said orbifold eigensets are to be basically of the same nature and behavior; except that one of these said eigensets is to work to bear a higher number of directly associated spatial dimensions, that are here to be proximal local to the topological stratum of the said orbifold eigenset, -- than the number of spatial dimensions that are here to be directly associated with the proximal local topological stratum of the other stated orbifold eigenset.  In this particular case; that orbifold eigenset, that is here to work to bear a greater number of spatial dimensions, -- will consequently tend to work to bear a greater flow, in the rate of the perturbation of its directly corresponding Chern-Simons Invariants -- when this is here to be taken, over that process, in which such an earlier implied covariant tense of a Hamiltonian eigenmetric is here to occur. Sincerely, Samuel David Roach.

Rate Of Flow In the Perturbation Of Chern-Simons Invariants

Let us initially consider two different given arbitrary orbifold eigensets, that are both to work to bear the same scalar amount of cohomology-related generation (to where, this will tend to reverse-fractal into both orbifold eigensets, working to be associated with the same scalar amount of charge.)  Both of these just mentioned orbifold eigensets, are here to be  basically of the same nature and behavior, except that one of these said orbifold eigensets is to work to bear a greater scalar amplitude, in the rate of the flow of the perturbation of its directly corresponding innate Chern-Simons Invariants, than the other said orbifold eigenset.  Based upon the directly previous stipulation, that orbifold of this particular case -- that is here to work to bear a greater scalar amplitude, in the rate of the flow of the perturbation of its directly corresponding innate Chern-Simons Invariants, will Tend to bear a higher scalar amplitude in the conglomerate rate of its directly associated i*PI(Del) Action, than the other of the two here mentioned orbifold eigensets, that was stated here, in this particular case.
I will continue with suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

The Polyakov Action And Hyperbolic Approach

The slower that the rate is, of any given arbitrary superstring of discrete energy permittivity, when this is here to be taken in its relationship to the motion of electromagnetic energy, the lower that its directly corresponding Lorentz-Four-Contraction will consequently tend to be.  The lower the Lorentz-Four-Contraction is to be, for any given superstring of discrete energy permittivity -- the higher that its directly corresponding Polyakov Action will then tend to be.  The higher that the respective Polyakov Action will tend to be, for any given superstring of discrete energy permittivity -- the greater that the scalar amplitude will tend to be, of the hyperbolic approach of the correlative respective second-order light-cone-gauge eigenstates, that are of the proximal local self-same discrete quantum of energy, -- as such said respective second-order light-cone-gauge eigenstates, are here to work to interconnect the directly corresponding Fadeev-Popov-Trace eigenstate that is of the self-same discrete quantum of energy, To the initially stated superstring of discrete energy permittivity, of such a particular given arbitrary case scenario.  To Be Continued!  Sincerely, Samuel David Roach.

Altering Rate Of i*PI(del) Action

When a given arbitrary mass-bearing orbifold eigenset is to be altering in its acceleration, when this is here to be taken in its relationship to the velocity of electromagnetic energy -- then, the correlative i*PI(del) action that is here to be directly corresponding to the said respective given arbitrary mass-bearing orbifold eigenset, will consequently tend to be altering in its rate.  Sincerely, Sam Roach.

Increasing Relative Velocity And Rarita Structure Eigenstates

Let us initially consider an orbifold eigenset, that is here in this case to consist of at least in part -- the presence of mass-bearing superstrings of discrete energy permittivity.  Let us next say -- that the said orbifold eigenset, is to be accelerating up to nearly the rate of light speed.  As the said orbifold eigenset is to be increasing in its relative velocity, over an evenly-gauged Hamiltonian eigenmetric -- it is then to bear increasingly more mass, -- even though the overall specific Ward-Neumman constraints of the said eigenset's physical bounds are to if anything decrease.  This then works to indicate, that, as the so-eluded-to set of superstrings that are here to operate to perform a specific function, is to move at a relatively increasing rate, when this is in comparison to light that is here to go even faster -- that the density of the mass of the said orbifold eigenset is then to increase as well.  This will then work to indicate the physical conditions of an increased density, as to what are here to be the correlative centralized knotting of the proximal local Rarita Structure eigenstates.  It is the Rarita Structure, that works to convey both the vibrations of gravity, as well as the multivarious inflections in the conveyance of the ever changing forms of the four main physical forces of nature.
I will continue with the suspense later!  To Be Continued!  Sincerely Samuel David Roach.