Conformal Repulsion/Conformal Attraction

 Let us, at first, consider two different initially covariant homotopically dispersed Hamiltonian Operators, that are here to bear a tense of a magnetic inter-relationship between one another. As one would more than likely presume; Both of such stated individually taken Hamiltonian Operators, are here to work to bear, both a general tense of angular momentum, and a general tense of spin-orbital momentum. It basically logically follows, therefore, that both of such said individually taken Hamiltonian Operators, will thereby work to bear a simultaneously spontaneous general tense, of both the exhibition-related display, of both a Euclidean Expansion, as well as exhibiting the display of an attributed Clifford Expansion, as taken in a respective covariant manner, via the vantage-point, of a central co-differentiable coni-axion. There is to logically be, amongst any set of magnetically interactive covariant co-differentiable Hamiltonian Operators, that are here to work to bear any viable tense of a Yukawa-Related Coupling between one another, both a general tense of conformal repulsion, and a general tense of conformal attraction -- of which are here to work to help facilitate their viable covariant differential association, at the substring-related level. At times, one may may stipulate, that the quotient between the respective correlative mathematical expression for the earlier implied Clifford Expansion, as divided by the respective correlative mathematical expression for the earlier implied Euclidean Expansion, as this is all multiplied by (-i/PI); -- may often be a potential mathematical way, of considering how to work to describe, the conformal repulsion, that is here to exist, between these two different stated covariant Hamiltonian Operators. Furthermore; At times, one may stipulate, that the product between the respective Mathematical Expression for the earlier implied Clifford Expansion, as multiplied by the respective mathematical expression for the earlier implied Euclidean Expansion, as this latter stipulation is all multiplied by (i*PI); -- may often be a potential mathematical way, of considering how to work to describe, the conformal attraction, that is here to exist, between these two different stated covariant Hamiltonian Operators. So; When one is to mathematically couple the earlier inferred "conformal repulsion" with the earlier inferred "conformal attraction," one will get the respective mathematical resultant, of simply the correlative "squared state" of the Clifford Expansion, of which may often have a tendency of simply working to indicate by this, that the Fourier-Related-Progression of the covariant planar gauged-action, that is to result between the two stated Hamiltonian Operators, will consequently involve the general physical condition, in which these two Hamiltonian Operators, will thence be exhibiting a steady-state transversal tense of conformal invariance, in which these Operators will resultantly be simply spinning/vibrating at a relativistically fixed locus, at a covariant internal reference-frame, to where these two inferred net eigenstates of composite discrete energy, will neither be moving away nor towards each other, at this point in translational development, since their potential repulsion/attraction characteristics, will, at this point in interaction, have the tendency, of being sufficiently countered amongst each other, since the respective correlative tangential wave-tug between them, will now be equally countered by the respective correlative co-tangential wave-tug between them. This is as such a general type of a case scenario, is here to be taken, at a level that is Poincare to the respective region, that is immediately external to the kinematic interplay, that is Yukawa, amongst the eminent electrodynamic magnetism, that is to be exhibited between these two earlier inferred respective types of Hamiltonian Operators. I WILL CONTINUE WITH THE SUSPENSE LATER! SAMUEL ROACH.