The Light-Cone-Gauge And Fed-In Mini-Stringular Segmentation

Let us initially compare two different genre of light-cone-gauge eigenstates.  One is of a Yang-Mills light-cone-gauge topology, while the other one is of a Kalutza-Klein light-cone-gauge topology.  The light-cone-gauge eigenstate that is of a Yang-Mills topology, is non-abelian in its general geometry.  Whereas, the light-cone-gauge eigenstate that is of a Kalutza-Klein topology, is abelian in its general geometry.  The light-cone-gauge eigenstate of this given arbitrary case -- that is of a non-abelian nature, works to bear second-order eigenstates that are of a relatively sinusoidal Laplacian-related composition, along the general region of the Lagrangian-based path in which these are delineated over the course of BRST. Whereas, the light-cone-gauge eigenstate of this given arbitrary case -- that is of an abelian nature, works to bear second-order eigenstates that are of a relatively supplemental Laplacian-related composition, along the general region of the Lagrangian-based path in which these are delineated over the course of BRST.  As the two so-eluded-to first-order light-cone-gauge eigenstates are to be in the process of going through an iteration of BRST that is both covariant, codifferentiable, and codeterminable, via the vantage-point of a central conipoint -- the correlative  individually taken Polyakov Action eigenstates, are to here to work to form the activity of a hyperbollic Clifford Expansion, that is to be involved with a euler-based acceleration of the directly corresponding feeding-in of mini-stringular segmentation --that is to exist for both of the correlative dually considered light-cone-gauge eigenstates, and their directly corresponding individually taken superstrings and counter strings.  The mentioned Yang-Mills-related light-cone-gauge eigenstate, during BRST, is to bear its correlative gauge-bosons -- that are to pluck each second-order light-cone-gauge eigenstate -- at those respective sinusoidal-based "troughs" at which the said gauge-bosons are to "pluck" the light-cone-gauge eigenstate like a harp.  Whereas, the mentioned Kalutza-Klein-related light-cone-gauge eigenstate, is to bear certain respective given arbitrary loci of encoded singularity -- at which their correlative and directly corresponding gauge-bosons are to "pluck" the corresponding second-order light-cone-gauge eigenstates like a harp.  Yet, as the so-eluded-to mini-stringular segmentation -- that is respective to the said Kaluza-Klein-related light-cone-gauge eigenstate -- is being fed-into the said eigenstate during BRST, -- this will work to form the equivalence of mini-troughs, at which the said respective gauge-bosons are to "pluck" the needed loci of the correlative abelian light-cone-gauge eigenstate, in so as to form Schwinger-Indices that act as gravity waves.
I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.