Wednesday, February 8, 2017

Core-Field-Density And Substringular Fields, Part One

Let us initially consider a given arbitrary bosonic superstring of discrete energy permittivity, that is taken at the Poincare level -- that is Gliosis to the topological substrate of the so-stated superstring.  Let us think here, in terms of the density of the topological surface -- that is at this general respective tense of locus.  The density that would exist here, under the Ward-Caucy-based conditions of such a so-eluded-to Laplacian-based transform, of such a so-eluded-to surface -- would approach infinity at the so-stated general proximal considered locus.  Next, let us consider the just mentioned superstring -- to be of a respective given arbitrary orbifold eigenset.  An orbifold eigenset is a set of one or more discrete quanta of energy -- that operate in so as to perform one specific function.  The partial of such a discrete quanta of energy -- that is specifically of basically the pointal-based characteristic of discrete energy permittivity -- is the perverbial superstring or superstrings, that work to comprise such a said orbifold eigenset.  The partial of such a discrete quanta of energy -- that is specifically of basically the wave-based characteristic of discrete energy permittivity -- is the perverbial superstringular counterpart  or superstringular counterparts, that work to comprise such a said orbifold eigenset.  The partial of such a discrete quanta of energy -- that is specifically of basically the pointal-based characteristic of discrete energy impedance -- is the perverbial Fadeev-Popov-Trace eigenstate or Fadeev-Popov-Trace eigenstates, that work to comprise such a said orbifold eigenset.  The partial of such a discrete quanta of energy -- that is specifically of basically the wave-based characteristic of discrete energy impedance -- is the perverbial first-ordered light-cone-gauge eigenstate or first-ordered light-cone-gauge eigenstates, that work to comprise the said orbifold eigenset.  Any given arbitrary discrete quantum of energy, will not be at the exact same relative spot -- over the course of two immediately consecutive iterations of group-related instanton.  Unless a given arbitrary orbifold eigenset is of only one discrete quantum of energy -- such a respective given arbitrary orbifold eigenset, will not work to bear a density that approaches infinity as quickly, as an individually taken superstring that is to be taken at the Poincare level will approach infinity -- when such a density is taken Gliosis to the topological substrate of such a so-stated respective so-eluded-to superstring or substringular eigenmember.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

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