Gauge-Boson Sliding

During that general activity of the decompactification that happens during the Polyakov Action -- upon any one given arbitrary discrete quantum of energy, over the course of BRST -- the correlative gauge-bosons that are to work to "pluck" the directly corresponding light-cone-gauge eigenstates, are to then be in the process of sliding along the topological surface of the hyperbollic Clifford Expansion, that is to here be Yukawa to the core-field-density of the so-eluded-to light-cone-gauge eigenstates, that are to here be directly associated with the so-eluded-to discrete quantum of energy that is to here be undergoing the so-eluded-to eigenstate of the said Polakov Action.  For the remainder of that increment of BRST, in which the said gauge-bosons are to be in the process of "plucking" the said light-cone-gauge eigenstates during the said Polyakov Action eigenstate, -- the said gauge-bosons, of which have just slid across the topological surface of the correlative light-cone-gauge eigenstates that are to have just been hyperbollically expanding in their core-field-density, -- are to then to tend to work to do what one would normally think of as the actual "plucking" action of the said gauge-bosons -- in so as to produce those Schwinger-Indices, that are to here act as the resultant gravity waves.  To Be Continued!  Sincerely, Samuel David Roach.