A Little Bit As To The Clifford Expansion And The Kahler-Metric

Superstrings -- over the process of the Polyakov Action -- decompactify to the inverse of their correlative Lorentz-Four-Contractions.  Let us here say that one given arbitrary superstring of discrete energy permittivity is to be Lorentz-Four-Contracted by a factor of two, at one respective setting.  Over the directly corresponding duration of the here correlative increment of relatively local BRST, the respective superstring that is to be contracted, over the correlative increment of the Polyakov Action, is decompactified via a Clifford Expansion, by a factor of 1.5*3^8 -- by the end of the so-stated correrlative duration of BRST.  Here is another example.  Let us say that a superstring is of a case that is of a Majorana-Weyl-Invariant-Mode, that is here relatively motionless -- in a terrestrial-based manner.  Then, over the ensuing respective given arbitrary duration of local BRST -- the superstring, over the correlative Polyakov Action, will be decompactified by a factor of 3*10^8 -- by the end of the so-stated respective increment of BRST.  So, when any respective given arbitrary orbifold eigenset is to undergo a relatively local increment of the Kahler-Metric -- after each correlative iteration of the directly corresponding individual increments of BRST -- each superstring of the so-stated orbifold eigenset, that is here to undergo the said ensuing process of the local Kahler-Metric, will reverse the decompactification of its scalar magnitude of relative length, as each of the so-eluded-to increments of discrete energy are pulled into the Ward-Neumman bounds of the directly corresponding holonomic substrate, that is of the correlative Klein Bottle eigenstate, that is of this case scenario.  This happens, as each directly pertinent bundle of both respective discrete energy permittivity and respective discrete energy impedance -- is pulled into the said substringular physical bounds of that holonomic substrate that is of the so-stated Klein Bottle eigenstate of this said case.  This works to cause the initial Clifford Expansion that happens to the scalar magnitude of the correlative superstrings, to be inversely oriented, temporarily -- as the said discrete energy is initially drawn as such -- per each individual increment of the directly corresponding Kahler-Metric, into the so-stated "bottle," to where as the said bundles of discrete energy are exiting the said "bottle" per each increment of the so-stated Kahler-Metric, in the process of the activity of each approached ending of group-related instanton -- to where the said "bundles" are brought back into their decompactified Ward-Neumman orientation, that is as an inverse to their so-eluded-to correlative Lorentz-Four-Contraction (per each individually considered superstringular unit) -- as the so-stated discrete energy is brought into the Regge Action-based "eigenmetrical" activity, that is utilized in so as to end each of such succeeding individually taken increments of group-related instanton.
To Be Continued!  I will continue with the suspense later!  Sincerely, Sam Roach.