Relative Asymmetric Tense Of Covariant Spin-Orbital Flow

 Let us initially consider two different vibrating covariant mass-bearing cohesive sets of discrete energy quanta, of which are here to both be bearing a tense of perturbation, in their directly corresponding Chern-Simons Invariants, due to the inferred consistent alterations in the correlative direction of their angular momentum, that is here to be due to their respective individually taken tense of spin-orbital momentum. Let us next work to consider the harmonic output, that is here to be tangentially flowing, from both of the respective individually taken inferred "teams" of mass-bearing energy, that are here to be directly associated, with such a dual tense of a covariant exhibition in display, of a perturbation in Chern-Simons Invariants. If each of such earlier stated mass-bearing cohesive sets of discrete energy quanta, are here to work to bear a mutual relative asymmetric tense of a covariant spin-orbital flow, in respect to one another, as these just inferred "teams" of mass-bearing energy, are here to be vibrating in a rotational manner, as these are here to be both radially and transversally propagated, along their covariant individually taken  Lagrangian-Based paths, as this is here to be considered, in respect to the flow of the adjacent eigenstates of the Rarita Structure, then, such an earlier inferred dual tense of a covariant display of an interaction, that is here to be exhibited by the inferred Yukawa-Related Coupling, that is here to be subtended by the Gliosis-Based gauge-like action of their externalized fields, as such a spontaneous eluded-to gauge-like action, is here to be initiated tangentially outward from the external field density, that is here to be expended in a covariant manner, at the Poincare level to the kinematic net Ward-Cauchy-Related force, that is here to be exhibited by the general gauged-metric, that is here to be eminent in its kinematic relationship, to the correlative regional proximal local Fourier-Related Transformation, that is here to be occurring to the respective dual tense of topological manifold, that is here to be appertaining to the interactive wave-tug, that is here to be incurred upon such a respective interactive dual tense of holonomic substrate, that has here to have been insinuated, as being of both a co-differentiable and of a co-determinable nature of a piecewise continuous spatial translation of holonomic motion, over time, as this is here to be considered as being spatially translated, as a dual tense of such an inferred Hamiltonian Operation, over the duration of a sequential series of group-related instantons; Then, -- there is here to be a relatively high probability, that this general tense of a case scenario, will often tend to reverse-fractal, into a Ward-Cauchy-Related situation, in which these two different inferred covariant "teams" of mass-bearing energy quanta, will consequently tend to often result, in working to have at least some sort of a magnetic attraction to one another. I WILL CONTINUE WITH THE SUSPENSE LATER!  TO BE CONTINUED! SAM. (1989).

A "Tad-Bit" Of A Straight Forward Interjetction

Since the more anti chiral, that the charges are to be, of two different given arbitrary cohesive sets of discrete energy quanta, when taken towards one another, -- the more highly attractive that these two different inferred sets of energy, are thence to be towards each other -- to where it follows then, that the more attractive that two different cohesive sets of discrete energy quanta, are to be towards one another, the more likely that such a pair of attracted mass-bearing eigenstates, will consequently tend to result in working to display the behavior, of exhibiting the general activity, of operating as an isotropic dual state of a covariant, co-determinable, and co-differentiable entity, that is here to be displaying the general behavior, as exhibiting a tense of group action. Consequently, as a reverse-fractal of what I just mentioned; when there is to be a more macroscopic tense, of a strong set of electrodynamic group-related attractions -- that are here to be bound in such a manner, to where such a said group-related state, is to act as one cohesive entity, on the whole, it may then be said here, as well, that such a herein inferred relatively "macroscopic" phenomenology, of such a given respective case scenario, is here to consequently tend to result in working to display the behavior, of exhibiting the general activity of operating as an isotropic state, by acting as a covariant, co-determieable, and co-differentiable entity, that is here to be displaying the general behavior, as exhibiting a tense of group action. I will continue with the suspense later! (1989). To Be Continued! Sincerely, Sam Roach. 

Tense Of Initial Magnetic Repulsion

 When one is to have the proximal local presence, of a set of cohomology-related eigenstates, that are here to work to each bear a tense of an initial magnetic repulsion, towards their immediately adjacent eigenstates, to where there is here to ensue, the gauged-action of a Gliosis-based Rayleigh scattering, that is here to occur, upon the overall net topological substrate, that is of such a stated set of cohomology-related eigenstates, there will consequently tend to occur, the general tendency, in which the earlier inferred eigenstates, that were initially to work to bear a tense of a magnetic repulsion, will alter into then working to bear a tense of magnetic attraction. (Cohomology-Related eigenstates, that are to work to bear the opposite parity, -- will tend to reverse-fractal into charges, that are here to work to bear the opposite chirality.)  To Be Continued! Sincerely, SAMUEL DAVID ROACH. (1989).

i*PI(del) Action -- Electrodynamics

Let us initially consider the workings of a given arbitrary charged mass-bearing orbifold eigenset (to where such a said respective eigenset, is here to work to bear a set of cohomology-related eigenstates, that are here to to be of an overall net perturbative nature), that is here to be undergoing a set of changes in its relative motion-- when this is here to be taken in relation to electromagnetic energy.:

The sequential accelerative operation of the net correlative i*PI(del) Action, tends to work in this respective given arbitrary general genus of a case, to bear an attractive force upon the ulterior externally delineated set of adjacent mass-bearing orbifold eigensets; Whereas -- the discrete quantum motion of the said orbifold eigenset Per the disturbance in space of the sequential operation of the net correlative i*PI(del) Action, tends to work in this respective given arbitrary general genus of a  case, to form a repulsive force upon the ulterior externally delineated set of adjacent mass-bearing orbifold eigensets. To Be Continued! Sincerely, Samuel David Roach.

Some More Stuff As To The Noether Current

The Noether Current is formed, by the flow of the multiplicit tense of "pressurized vacuum" -- that  the multifarious sets of cohomological eigenstates, tend to bear towards one another.  Sets of cohomological eigenstates that are of the opposite parity, tend to bear an inverted tense of a "pressurized vacuum" towards one another -- that tends to form a "suctioning" effect at the substringular level, -- that will consequently tend to form a tense of an attraction, between such sets of cohomology-related eigenstates, that are here to work to bear the opposite parity.  Whereas -- sets of cohomology-related eigenstates that are of the same parity, tend to bear a non inverted tense of a "pressurized vacuum" towards one another -- that tends to form a "conformal repulsion" effect at the substringular level, -- that will consequently tend to form a tense of a repelling, between such sets of cohomology-related eigenstates, that are here to work to bear the same parity.  Sincerely, Sam Roach.