More As To Relative Covariant Wobbling

Let us first take into consideration, two adjacent Fadeev-Popov-Trace eigenstates that are of the same given arbitrary universal setting -- that thence work to bear a covariant wobble of topological-based sway, that is of a  magnitude of 1.104735878*10^(-81)I degrees.  Let us now take into consideration, two other adjacent Fadeev-Popov-Trace eigenstates -- that are of another given arbitrary universal setting.  Let us say, that -- due to the manner as to the scalar magnitude of how different the distinction of mathematical difference is, between the first so-eluded-to universal setting towards the second so-eluded-to universal setting, that is as to how distinct the two implied universal settings are, (as to how "far-off" the two sets of adjacent Fadeev-Popov-Trace eigenstates, that are of two different respective universal settings, is), the two said sets of Fadeev-Popov-Trace eigenstates will here bear a covariant wobble of topological-based sway, that is of a magnitude that is arbitrarily of exactly three times the magnitude that the so-stated eigenstates that are of the same universal setting, will tend to bear, amongst each other. (3*1.104735878*10^(-81)I degrees.) (Yet, both individual sets of Fadeev-Popov-Trace eigenstates of this respective given arbitrary case scenario, will work to bear -- towards the other said eigenstate that is of the same universal setting -- the so-mentioned wobble of 1.104735878*10(-81)I degree angling towards the other of such eigenstates.)  This is due to the condition, that, when one is to have two sets of adjacent Fadeev-Popov-Trace eigenstates -- that are of two different respective universes -- the relative wobble, that is covariant from the first arbitrary set of such so-stated eigenstates, will bear a Clifford Expansion of its harmonic-based displacemnt, towards the second of such a so-stated arbitrary set of eigenstates, in such a case where there are here two given arbitrary different sets of adjacent Fadeev-Popov-Trace eigenstates -- that are encoded to belong to two different universes. So, depending upon the degree of as to how different the distinction is between one set of respective given arbitrary Fadeev-Popov-Trace eigenstates is towards another set of respective given arbitrary Fadeev-Popov-Trace eigenstates -- the more that the Clifford Expansion is to happen to the inter-binding Real Reimmanian-based Rarita Structure eigenlocus, that will here work to interdependantly inter-bind the Hamiltonian-based Lagrangian -- that is Gliosis as a mappable tracing, from the Laplacian-based Majorana-Weyl-Invariant setting of the first so-stated locus of one of such sets of Fadeev-Popov-Trace eigenstates towards the second locus of such sets of Fadeev-Popov-Trace eigenstates -- of this respective given arbitrary case.
I will continue with the suspense later! To Be Continued!  Sincerely, Sam Roach.