More About The Motion Of Gauge-Bosons

As second-ordered light-cone-gauge eigenstates are fed mini-string over the course of BRST in such a manner in so that the respective given arbitrary light-cone-gauge eigenstate may work to coordinate the respective superstring with its corelative Fadeev-Popov-Trace, the directly affiliated gauge-bosons that pluck the corresponding second-ordered light-cone-gauge eigenstates moves along with the directly affiliated motion that directly relates to the here related Clifford Expansion that happens over the said course of BRST that is associated with a superstring that is here being contracted during this given arbitrary case.  The flow of the motion of the mentioned gauge-bosons that "tags" along with the directly affiliated second-ordered light-cone-gauge eigentates is caused by the same general pulse of motion that works to cause the directly related kinematic response that forms the corresponding Polyakov Action eigenmetric that works to expand the length of a superstring to the inverse as to how the given arbitrary superstring is contracted to our perspective.  So, as a superstring is decompactified legthwise to the inverse as to how it is contracted to our perspective during the Polyakov Action -- that happens during a course of BRST,  of which is the main portion of the duration of group instanton -- the corresponding counterstring that is directly associated with the mentioned superstring is likewise decompactified to the same scalar degree.  Meanwhile, the corresponding gauge-bosons that pluck the corresponding second-ordered light-cone-gauge eigenstates in so that both gravity and Schwinger-Indices may occur kinetically flow in a manner that "tags-along" with the said light-cone-gauge eigenstates due to a synchronous norm-state projection that works to pull the said gauge-bosons in a manner that bears a relatively hyperbollic-based hermitian and bilateral isosymmetry with the acitivity that happens over the course of that Clifford Expansion that happens due to the activity of the said Polyakov Action eigenmetric that has here been eluded to.  The direclty prior -- when coupled with the wave-pull that is here associated with the Gliossi manner in which the gauge-bosons pluck the corresponding second-ordered light-cone-gauge eigenstates -- works to allow the said bosons to keep at their needed loci in a manner that is Poincaire to the topological surface of the mentioned eigenstates.  So, as the corresponding superstring and its counterpart is brought into its needed conditioin after BRST, the gauge-bosons are pulled out of the general locus of the direct field of their directly related light-cone-gauge eigenstates in a directoral basis that is Njenhuis to the forward-holomorphic genus of direction -- when relative to the holomorphic direction that the given arbitrary superstring is to travel in right after the directly associated iteration of group instanton.  I will continue with the suspense later!  Sam Roach.