Part 3 Of The Flow Of The I*PI(del) Action

 The heuristic permeation of the flow of the i*PI(del) Action, often tends to help in working to facilitate, the inverted dispersion, of spontaneously formed Chern-Simons Invariant metric-gauge eigenstates. Whereas; The dispersive restraint of the flow of the I*PI(del) Action, often tends to help in working to facilitate, the heuristic dispersion, of spontaneously formed Chern-Simons Invariant metric-gauge eigenstates. I WILL CONTINUE WITH THE SUSPENSE LATER! TO BE CONTINUED! SINCERELY, SAMUEL LDAVID ROACH. 

Gell-Mann Theorem -- Dispersion Of Homotopic Residue

 As in accordance with the Gell-Mann Theorem; -- When a given arbitrary Noether-Based mass-bearing cohesive set of discrete energy quanta is to spin, it will consequently tend to work to form a dispersion of homotopic residue. I WILL CONTINUE WITH THE SUSPENSE LATER! SINCERELY, SAM ROACH.

Homotopic Dispersion -- Riemann/Rayleigh Scattering

 When a given arbitrary tense of homotopic dispersion is to happen, via a Riemann Scattering, this will often have the general tendency, of working to form magnetism, of which will tend to reverse-fractal into electrodynamic charge.  Whereas; When a given arbitrary tense of homotopic dispersion is to happen, via a Rayleigh Scattering, this will often have the general tendency, of working to form a local tense of holonomic disorder, of which will tend to reverse-fractal into entropy. TO BE CONTINUED! SAMUEL.

Stronger Harmonic Superstring-Related Dispersion -- More Intensified Hermitian Cohomology -- More Isotropically Stable Electromotive Current

 The stronger that the harmonic superstring-related dispersion is to be -- The more intensified that the consequentially formed hermitian cohomology is to tend to be -- To, where; The more isotropically stable that the consequentially formed resultant electromotive current, is therefore to tend to end-up becoming. TO BE CONTINUED! SAMUEL. 

Relatively Analogous Heuristic/Inverted Dispersions Of Homotopic Residue

 Let us initially say, that one is here to be comparing two different relatively analogous cases, as to the dispersion of homotopic residue; -- Except, that one of such dispersions, is of a heuristic nature -- while -- the other of such dispersions, is of an inverted nature. The relativistic directional pulsation, of such a heuristic dispersion of homotopic residue, here, in this particular case scenario, may often tend to be equal to (-i) times the relativistic directional pulsation, of the inverted analogous dispersion of homotopic residue. I WILL CONTINUE WITH THE SUSPENSE LATER! SINCERELY, SAMUEL ROACH. (1989)

Heuristic Dispersion Of Conserved Homotopic Residue

 When a given arbitrary Noether-Based mass-bearing cohesive set of discrete energy quanta, is here to work to bear a perturbation, that is to be operationally directed Out of a state of gauge-invariance, when such an inferred alteration, is here to be incurred upon the topological manifold of such a stated set of discrete energy quanta, the entropy, that is here to be directly associated with this general type of a process, tends to work to bear a reductional tense, of a heuristic dispersion of conserved homotopic residue. TO BE CONTINUED! (PHS). I WILL CONTINUE WITH THE SUSPENSE LATER! SINCERELY, SAMUEL ROACH. (1989).

Smooth Homotopic Dispersion

 When a given arbitrary accelerating Noether-Based mass-bearing cohesive set of discrete energy quanta, is to work to exhibit the display, of a smoothly homotopic tense of a heuristic dispersion, it will often have the general tendency, of working to exhibit a relatively smooth emission, of entropic metric-gauge-related eigenstates. Furthermore; When a given arbitrary accelerating Noether-Based mass-bearing cohesive set of discrete energy quanta, is to work to exhibit the display, of a smoothly homotopic tense of an inverted dispersion, it will often have the general tendency, of working to exhibit a relatively smooth emission, of charge-related metric-gauge eigenstates. I WILL CONTINUE WITH THE SUSPENSE LATER! SAM.

Anharmonic/Harmonic Output -- Cevita/Wess-Zumino Interactions

 The heuristic dispersion of those entropic metric-gauge-related eigenstates, that are here to be formed, by the anharmonic output of perturbative Chern-Simons Invariants, works to be eminently associated, with the consequential resultant, of the Rayleigh tense of a general genus of a Cevita interaction. Whereas; The inverse-dispersion of those charge-like metric-gauge-related eigenstates, that are here to be formed, by the harmonic output of perturbative Chern-Simons Invariants, works to be eminently associated, with the consequential resultant, of the Riemann tense of a general genus of a Wess-Zumino interaction. SAMUEL.

Relatively High Dispersion Of Chern-Simons Invariants -- Relatively High Entropy

 Any given arbitrary Ward-Cauchy-related region, in which there is here to be a relatively high scalar amplitude of a dispersion of Chern-Simons Invariants, will consequently tend to be a Ward-Cauchy-related region, in which there will resultantly often tend to be a relatively high scalar amplitude of entropy. SINCERELY, SAMUEL ROACH.

Reversed Direction Of Net Spin-Orbital Momentum -- Reversed Direction Of Dispersion

 When a given arbitrary mass-bearing cohesive set of discrete energy quanta, is to spontaneously work to bear a reversal, in the direction of the directly corresponding net tense, of its directly corresponding spin-orbital momentum, -- this general type of a common occurrence, will often tend to result, in a consequentially occurring case scenario, in which there is here to be the ensuing display, of an exhibited reversal in the net direction, of the dispersion of those particular eigenstates, that are here to be expended outward and away From the proximal local field-density, that is to be of the said respective mass-bearing cohesive set of discrete energy quanta, which is here to be considered, over the general durational course, of that kinematic activity, in which those correlative respective tangentially flowing eigenstates, that are here to tend to be formed, by the enactment of the directly corresponding Chern-Simons-Invariants, are to be generated, in a relatively homotopic manner, over the span of a sequential series of group-related instantons. I WILL CONTINUE WITH THE SUSPENSE LATER! SINCERELY, SAM ROACH.

More As To Cohomology-Related Eigenstates/Emmited Eigenstates Of Dispersion

 The multiplicity of cohomology-related eigenstates, have a tendency of behaving, as the energy-related "facets," that are here to work to form a "latched" core viable physical field-like entity, that is here to be "tagged-along," by the projected trajectory, that is here to be exhibited, by the general consequential resultant motion, of discrete energy phenomenology, as it is to be spatially transferred through its directly corresponding Lagrangian, over the directly associated durational motion, that is here to work to bear a tense of a physical spatial dimensional translation, through the general medium of space-time-fabric, as this is here to be taken, over a correlative Fourier Transformation. Whereas; the multiplicity of the respective emmited eigenstates of Chern-Simons dispersion, tend to act in a manner, that is here to be tantamount, to a spatially translated ripple-like effect, that is here to be spatially transferred over time, as this is here to work to bear a tense, of a particular general genus of a propagated disturbance in space, that is here to bear a residual tense of a homotopic effect, upon the multiplicity of those oscillation-related vibrations, that are here to be potentially interactively viable, upon certain susceptible eigenstates, that are of a Ward-Cauchy-Related topological nature, as such a propagation of a time-wise euclidean/Clifford expansion, of such a tangential divergence, is to be tugged along the Rarita Structure, as such dispersion-related eigenstates, are here to be operationally carried-out, over a sequential series of (group-related) instantons. Sincerely, SAM ROACH.

More Diffeomorphic Externalized Shell -- Smoother Dispersion Of Emitted Chern-Simons Invariants

 The more diffeomorphic that the externalized shell of a given arbitrary mass-bearing cohesive set of discrete energy quanta is to be, the smoother that the correlative dispersion of the directly corresponding emitted Chern-Simons Invariants will consequently tend to be -- that is here to be formed, by the general process in which such an inferred tense of a cohesive set of discrete energy quanta, is here to be spatially translated through a respective Lagrangian-Based path, as this is here to be taken, via a directly associated Fourier Transformation, in the general process, by which such an inferred symmetrically shaped holonomic entity, is here to be transferred from one spot to another, over a correlative duration to time. SAMUEL DAVID ROACH.

"Phased-Out" Communicable Message (Signal) -- Dispersion

 When any given arbitrary electrodynamicly transmitted communicable signal-related message --  that is here to be delineated from one general proximal locus to another -- is here to have ended in its allocation, by the general process, in which such a said message is here to have been "phased-out" of being sent, to wherever it was initially distributed to; -- it follows then, that one may consequently say, that the respective given arbitrary cohesive set of vibrational oscillations, that were here to have initially been in the process of working, via a directly corresponding propagated electrodynamic-related spatial transmission in time and space, in order for such a said/inferred signal, to have been able to have been sent to such an inferred initially designated destination, in order to be able to transfer or carry the initially delineated given arbitrary respective electrodynamicly communicable message -- at the point in time in which such a said cohesive set of communicable vibrational oscillations, are to have been ended in their propagational spatial translation -- that the signal that is to here to have just been "disbanded," may thereby be described of, as having had gone through the general process, of electrodynamic "dispersion."

I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach. (1989).