Why The Light-Cone-Gauge Is Named What It Is

During the Polyakov Action, superstrings of discrete energy permittivity unstretch in terms of their length (for one-dimensional superstrings) or in terms of their circumference (in terms of two-dimensional supserstrings) to the inverse extent that the said mentioned superstrings are not totally contracted.  Throughout the duration of BRST -- which is when both the Bette Action and the Polyakov Action happen -- mini-string wave import is fed into the general locus of field partial in which the related first-ordered-light-cone-gauge eigenstate is existent at during the said duration of BRST.  The wave import that here describes the corresponding light-cone-gauge eigenstate, during the activity in which the Polyakov Action is happening, thus forms a cone-shaped field that may be mapped when one integrates the general region in which the mentioned given arbitrary light-cone-gauge eigenstate is working to provide a basis for a substrate in which gauge bosons may pluck these like a harp so as to form the necessary vibrations -- Schwinger Indices -- that are needed to covariantly inter-relate norm projections with externalized superstrings so that discrete energy may kinematically interact with other discrete energy.  The Polyakov Action happens to the inverse extent of Lorentz-Four-Contractions, and, Lorentz-Four-Contractions happen based on the relationship of superstrings to the motion and existence of light (quantized photons).  The integrated mapped sub-metric generalized partial field that exists as both a basis of substringular interaction and a basis for the springing of superstrings into that Ultimo;n Flow that gauges where a superstring is to be relocated during its next iteration forms a sloped conical concavity that apexes at the conipoints where the related mini-string segments are interwovenly tied in a kinematic manner at the related Fadeev-Popov-Trace that is most directly associated with the corresponding superstrings that are here undergoing Polyakov Action.  The corresponding mini-string segments are constantly fed wave import where the related light-cone-gauge eigenstate is kinematically differential during an eigenmetric of Polyakov Action.  The slope of a light-cone-gauge eigenstate during the Polyakov Action is hermitian when a corresponding superstring is orientable.  The light-cone-gauge is a gauge in the manner that it works to provide an initial basis for the determination of the redelineation of superstrings that most directly correspond with the related first-ordered-light-cone-gauge eigenstates.  There is a lot more that I wish to describe in relation to this.  I will continue with the suspense later!  Sincerely, Sam Roach.