As To The Directional-Related Alteration, Of The Dispersion Of Chern-Simons Invariants

 When any given arbitrary mass-bearing cohesive set of discrete energy quanta, is to reverse the directional import of the wave-tug-related indices, as its directly corresponding spin-orbital momentum is to reverse in its directional covariant flow, when this is in terms of the cohomology-related eigenstates, that are here to be generated, -- to where the tangential tense of the nodal flow, that is of the correlative superstring-related field eigenstates, is to reverse in its covariant directional import -- the consequential flow of the directly associated dispersion eigenstates, that are here to be displayed as the outgoing physical emission of the directly associated Chern-Simons Invariants, are to flow in such a manner, as it is thence to bear a reversal in its physical mode of perturbation-related gauge-metrics, -- to where this will thereby often tend to reverse-fractal, into resulting into a directly associated case scenario, by which there is here to be the kinematic spatial translation, over a span of time, of a spontaneous reversal in the correlative charge, that is here to be most associated with the magnetism, that is here to be eminent in expression, at the covariant Fourier-Related internal reference-frame, that is here to be heuristically delineated, as being  at the Poincare level, to the topological surface of the external shell, that is here to be most associated with the particular given arbitrary respective mass-bearing cohesive set of discrete energy quanta, that is here to be of such a general example, of a given arbitrary case scenario, in which a charge is here to be in the general process, of reversing in its polarity, over a given arbitrary proscribed duration of time. Again; Chern-Simons Invariants are only "invariant" for a mass-bearing cohesive set of discrete energy quanta (a "team" of energy quanta), when the motion of the said directly associated mass-bearing cohesive set of discrete energy quanta, is to not change in its mode, in relation to the motion of light. Later On! SAM.