About Light-Cone-Gauge Topology

The topology of the light-cone-gauge is very important -- when one is to consider the potential genus of any given arbitrary phenomenon that one is to determine and/or extrapolate in the substringular.  The overall light-cone-gauge of any one given arbitrary superstring may be termed of as a first-ordered light-cone-gauge.  Although one may often consider the topology of a first-ordered light-cone-gauge as a genus of the "topography" of an attribute that exists in the substringular, the topology of second-ordered light-cone-gauge eigenstates works to act as more of a "topographical" condition of the same general conditionality of the so eluded to substringular operation that always exists, in correlation to the Hamiltonian operation of superstrings -- as the so-stated superstrings of discrete energy permittivity work to function as Hamiltonian operators in the substringular, in their multiplicit activities that act in so that superstrings may be put into the course of the activity of what I have termed before as Ultimon Flow.  It is the second-ordered light-cone-gauge eigenstates that get "plucked" by their directly corresponding gauge-bosons in so as to form those vibrations that may be thought of as second-ordered Schwinger-Indices -- that flow, via the multiplicit eigenstates of the Rarita Structure, in so as to form the operational indices of the activity of the Ricci Scalar.  It is these just eluded to vibrations that work to form the eminent corresponding inter-relationship between superstrings of discrete energy permittivity and Fadeev-Popov-Trace eigenstates of discrete energy impedance with gravitational-based particles, so that gravity may work upon the countless phenomena of the substringular -- so that phenomena may be brought together enough so that phenomena may have a coterminable, covariant,  and a codifferentiable influence upon the other eluded to phenomena that exists along the contour of the fabric of the space-time-continuum.  This previously eluded to "topographical" topology, that would here appertain to the Gliossi-based surface of the so-stated second-ordered light-cone-gauge holonomic substrate -- at the Poincaire level -- may be either non-abelian in nature or Yang-Mills, or, it may be abelian in nature or Kaluza-Klein.  Any given arbitrary non-abelian light-cone-gauge topology of the said second-ordered light-cone-gauge eigenstates that exist are delineated -- in a non-time-oriented manner -- in a sinusoidal manner.  Whereas, any given arbitrary abelian light-cone-gauge topology of the said second-ordered light-cone-gauge eigenstates that exist are delineated -- in a non-time-oriented manner -- in a supplemental manner, given the intrinsic space-time-curvature that is Gliossi to the eluded to light-cone-gauge eigenstates just mentioned.  (Not to be confused with being supplemental in the manner of a Wilson Line-based genus.)  Think about it.  If one had a elastic straight pole to push something, it would be more able to bear a wave-tug/wave-pull upon whatever it pushed upon.  Yet, if one had a curvy elastic pole, it would be less able to bear a wave-tug/wave-pull upon whatever it pushed upon.  This gives part of what is meant, in general, by either an abelian, or, a non-abelian, geometrical genus.  ( A little heads-up.)  I will continue with the suspense later! Sincerely, Sam Roach.