I'm Getting The Hang of the Light-Cone-Gauge, Part One

First of all, this corrective material is a preview as to the nature of OPE gauge-bosons.  Here is some of an outlook as to both how the light-cone-gauge is constructed, and, as to how the light-cone-gauge works, as well.  Let us say that we are initially dealing with a first-ordered light-cone-gauge eigenstate that is directly affiliated -- in a Gliossi-based manner -- with one respective given arbitrary two-dimensional superstring of discrete energy permittivity.  Each of the ten second-ordered light-cone-gauge eigenstates that work to comprise the here eluded-to first-ordered light-cone-gauge eigenstate here in question, is comprised of twelve mini-stringular-based segments -- that work to interconnect one Fadeev-Popov-Trace eigenstate with its directly corresponding two-dimensional superstring, that has been here stated for this given case scenario. This bundle of twelve mini-stringular segments bear a maximum tense of compactification at the Poincaire level, when taken at their topological surface, at the very beginning of any specific iteration of group instanton (at the start of the said iteration of BRST).  As the respective directly associated gauge-metrical activity of the Polyakov Action, that is acting upon the said superstring, is undergoing the here eluded-to operation, there is mini-stringular holonomic substrate that is fed into the so-stated second-ordered light-cone-gauge eigenstates, in order for the directly affiliated superstring to decompactify to the inverse degree as to the manner of operation that the directly affiliated Lorentz-Four-Contraction will here work to bear its Gliossi-based compactification upon the said two-dimensional superstring.  As the so-stated mini-string-based holonomic substrate, or, as the core-field-density of a substringular-based nature, is being fed into the ten directly affiliated second-ordered light-cone-gauge eigenstates, that work to comprise the said first-ordered light-cone-gauge-eignestate, of this given case, the said second-ordered light-cone-gauge eigenstates will then work to begin to bear a relative side-to-side topological-based sway -- that here works to bear a torsioning, that is initailly pulled radially to the equivalent scalar magnitude of two thicknesses of mini-string to the relative right, while then being pulled radially to the equivalent scalar magnitude of two thicknesses of mini-string to the relative left -- of whatever the general direction as to what is the vantage-point of the directly corresponding superstring's relative holomorphic-based direction.  If the superstring of this case here is of a Yang-Mills light-cone-gauge topological nature, then, each corresponding second-ordered light-cone-gauge eigenstate is -- over the whole general iteration of BRST that I have here eluded-to, is sinusoidal, in a non-time-bearing manner, to bear 30 respective troughs and 30 respective peaks -- throughout the whole here eluded-to iteration of BRST, in spite of the here eluded-to Gliossi-based inter-relation of that Clifford Expansion that would happen here.  The directly corresponding gauge-bosons that will here work to "pluck" the second-ordered light-cone-gauge eigenstates of this case, will here only tend to pluck at the troughs of the sinusoindal relatively standing waves that I have here eluded-to.
I will continue with the suspense later!  To Be Continued!  Sam Roach.