Universal Setting As To Schwinger-Indices

If two different individually taken Schwinger-Indices work to form a helicity, that is to directly involve a supplemental eigenbase of Ward-polorization -- when this is taken in retrospect to the propagation of the so-stated Schwinger-Indices or gravity waves, in a covariant interdependence to one another over a sequential series of group-related instantons -- then, this will work to indicate that the discrete energy quanta that had worked to form the two different distinct respective given arbitrary Schwinger-Indices, are to here tend to be of the same universal setting.  Yet, if two different individually taken Schwinger-Indices work to form a helicity that is to directly involve a complementary eigenbase of Ward-polarization -- when this is taken in retrospect to the propagation of the so-stated Schwinger-Indices, or gravity waves, in a covariant interdependence to one another, over a sequential series of group-related instantons -- then, this will work to indicate that the discrete energy quanta that had worked to form the two different distinct respective  given arbitrary Schwinger-Indices are of two different universes.  Yet, if the two different individually taken Schwinger-Indices that are of such a related case scenario -- are to work to form a helicity that is to directly involve a Yukawa-based torsioning, that is of the holonomic substrate of the so-eluded-to gravity waves -- that is not Ward-polarizable at one set convergent locus as to where  the Gaussian normalization of the vibrational indices that are at the Poincare level to the interfacing of those covariant Hamiltonian-based indices -- that are Gliosis to the interaction of the eigenstates of the topological stratum that is of the said holonomic substrate, that is of the so-stated Schwinger-Indices, then, if the ordering of the chirality that is taken along the topological interfacing of the so-eluded-to Gliosis-based contact of the one tense of the Fourier-based interactive helicity of what may here be arbitrarily called the initial Schwinger-Index in this respective given arbitrary case scenario, is of an even chirality with respects to the delineation-related angle-based positioning of what may here be arbitrarily taken as the second stated Schwinger-Index of such a respective given arbitrary case, then, the directly associated discrete quanta of energy that had worked to form both of the said Schwinger-Indices, are going to tend to be of the same universal setting.  Yet, if the two different individually taken Schwinger-Indices of such a related case scenario are to work to form a helicity that is to directly involve a Yukawa-based torsioning, that is of the holonomic substrate of the so-eluded-to gravity waves -- that is not Ward-polarizatlbe at the Poincare level to the interfacing of those covariant Hamiltonian-based indices that are Gliosis to the interaction of the eigenstates of the topological stratum that is of the said holonomic substrate of the so-stated Schwinger-Indices, then, if the ordering of chirality that is taken along the topological interfacing of the so-eluded-to Gliosis-based contact of the one tense of the Fourier-based interactive helicity of what may be arbitrary called the initial Schwinger-Index in this respective given arbitrary case scenario, is of an odd chirality with respects to the delineation-related angle-based positioning of what may here be arbitrary taken as the second stated Schwinger-Index of such a respective given arbitrary case, then, the directly associated discrete quanta of energy that had worked to form both of the said Schwinger-Indices are going to tend to be of two different universal settings.  I will continue with the suspense later! To Be Continued!  Sincerely, Sam Roach.