Solution 4 To Test 2 Of Course 20

4)  Superstrings of discrete electromagnetic energy permittivity, bear a Yang-Mills light-cone-gauge topology.  Light-Cone-Gauge eigenstates exist, per individually taken iteration of the multiplicit Polyakov Action -- which is here in this case, not working to consider the directly corresponding Clifford Expansion that would here be Yukawa to the said light-cone-gauge eigenstate, right in-between the multiplicit Fadeev-Popov-Trace eigenstate and its correlative multplicit superstring of discrete energy permittivity.  A Yang-Mills light-cone-gauge topology, is one in which the said eigenstate is of a non-abelian topololgy.  What this means here, is that a Yang-Mills light-cone-gauge topology -- is comprised of by mini-stringular segmentation that subtends between the respective Fadeev-Popov-Trace and its correlative superstring, in a manner that is of sinusoidal relatively standing waves, that are here being "fed-into" the proximal locus of the region at which the light-cone-gauge is being iterated -- during the so-eluded-to Polyakov Action  eigenstate.  As this Polyakov Action happens, gauge-bosons act -- in so as to "pluck" the directly corresponding second-order light-cone-gauge eigenstates, at the "troughs" of these just mentioned states.  I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.