Some Stuff About A Certain Genus of the Clifford Expansion

Right at the start of one given arbitrary iteration of BRST -- the field that is formed by the Ward-Neumman bounds of the mappable tracing of the topological holonomic substrate, of any respective given arbitrary first-ordered light-cone-gauge and its directly corresponding  given arbitrary  arbitrary one-dimensional superstirng of discrete energy permittivity or any two-dimensinoal superstring of discrete energy permittivity, will work to form a certain manner of a morphological setting.  This morphology, or shape of such a field -- that would here directly involve a one-dimensional superstring -- at the beginning of the said iteration of BRST, will be of as a wedge-like shape.  The morphology, or shape of such a field -- that would here directly involve a two-dimensional superstring -- at the beginning of the said iteration of BRST, will be of as a double-rhombus that is pulled toward a central annulus.  The said descriptions may be observed as the so-eluded-to second-ordered light-cone-gauge eigenstates of such directly associated cases are approaching, in a no-time-oriented manner, the said superstrings of discrete energy permittitivy.  This helps, in part, to cause the condition that one-dimensional superstrings of discrete energy permittivity tend to form conical world-sheets, while, two-dimensional superstrings of discrete energy permittivity tend to form toroidal world-sheets.  The ensuing metric of the Polyakov Action works to make these given arbitrary respective fields just mentioned to assymptote into a hyperboloid -- in the process of such a genus of a Clifford Expansion.