Torsioning Of Second-Ordered Light-Cone-Gauge Eigenstates

Any discrete quantum of energy, will either have an abelian light-cone-gauge topology, or, it will have a non-abelian light-cone-gauge topology -- over the course of any one respective given arbitrary iteration of BRST, during the course of any one given arbitrary respective iteration of instanton.  Any discrete quantum of energy that has an abelian light-cone-gauge topology, will tend to have more of a Laplacian lay-out -- of working to bear supplemental second-ordered light-cone-gauge eigenstates.  The lay-out of these just inferred eigenstates, will basically be of a linear eigenbase -- that is being fed-in mini-stringular segmentation, over the course of that Clifford Expansion that is to here be directly involved with the Fourier-based translation of that Polyakov Action eigenstate,  that is to happen to any respective superstring that is of a Kaluza-Klein light-cone-gauge topology.  In contrast -- the lay-out of those second-ordered light-cone-gauge eigenstates that are of a non-abelian light-cone-gauge topology, -- that work to comprise the wave-based format of any given arbitrary discrete quantum of energy impedance, is placed in a Laplacian-based sinusoidal manner -- during the directly associated iteration of BRST, which is of the correlative respective iteration of instanton.  This so-stated genus of light-cone-gauge topology, is also being fed-in mini-stringular segmentation, during the course of that Clifford Expansion that is correlative to the Polyakov Action eigenstate -- that is to here be directly appertaining to any respective given arbitrary iteration of instanton.  Since any so-eluded-to Yang-Mills light-cone-gauge topology (non-abelian), works to involve a distinctly sinusoidal tense of core-field-density, that is Gliosis at the Poincare level to the topological stratum of the directly corresponding second-ordered light-cone-gauge eigenstates -- this will then work to cause the condition, that such wave-based eigenstates, that are correlative to discrete quanta of energy impedance, will likewise tend to cause the condition, that, superstrings that are of a Yang-Mills nature, will tend to bear light-cone-gauge eigenstates that are more prone to being torqued -- than superstrings that are of a Kaluza-Klein light-cone-gauge topology.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.