Abelian Advantage

Let us initially consider two different physical phenomenologies, of which are to here work to form two different individually taken forces -- to where the two said different phenomena are to here be situated, in so as to press upon another given phenomenon, to where the phenomenon that is thus to be acted upon by this so-eluded-to process, is to be relatively right in-between the pushing action of the two said forces, that are to here be acting in exactly the relative opposite Ward-based direction -- over a set group-metric.  Let us next say -- that the Yukawa-based ends of both of the two said forces, that are to here be acting upon the third so-stated phenomenology that is to be positioned here right in-between the two so-stated forces, that is to here be most Gliosis-upon the holonomic substrate that is to be acted upon by both of the two said forces, that are acting in so as to work to potentially counter one another, are here to be working to bear the same general genus of both morphology, elastic modulus, and fractal modulus -- during the initially stated group-metric.  Then, the individually taken force, that is to here bear the highest scalar amplitude of an abelian geometry in the holomorphic direction of the immediate proximal locus, -- will tend to be the one of the two forces of such a given arbitrary case scenario, that will win-out as that eigenstate, that will then tend to work to bear more of an influence, as to the process of then working to guide the direction by which the initially relatively central thus acted upon phenomenon will move into next.

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