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.